%% Papers Published
@article{fds376029,
Author = {ATLAS Collaboration},
Title = {A detailed map of Higgs boson interactions by the ATLAS
experiment ten years after the discovery.},
Journal = {Nature},
Volume = {607},
Number = {7917},
Pages = {52-59},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {July},
url = {http://dx.doi.org/10.1038/s41586-022-04893-w},
Abstract = {The standard model of particle physics<sup>1-4</sup>
describes the known fundamental particles and forces that
make up our Universe, with the exception of gravity. One of
the central features of the standard model is a field that
permeates all of space and interacts with fundamental
particles<sup>5-9</sup>. The quantum excitation of this
field, known as the Higgs field, manifests itself as the
Higgs boson, the only fundamental particle with no spin. In
2012, a particle with properties consistent with the Higgs
boson of the standard model was observed by the ATLAS and
CMS experiments at the Large Hadron Collider at
CERN<sup>10,11</sup>. Since then, more than 30 times as
many Higgs bosons have been recorded by the ATLAS
experiment, enabling much more precise measurements and new
tests of the theory. Here, on the basis of this larger
dataset, we combine an unprecedented number of production
and decay processes of the Higgs boson to scrutinize its
interactions with elementary particles. Interactions with
gluons, photons, and W and Z bosons-the carriers of the
strong, electromagnetic and weak forces-are studied in
detail. Interactions with three third-generation matter
particles (bottom (b) and top (t) quarks, and tau leptons
(τ)) are well measured and indications of interactions with
a second-generation particle (muons, μ) are emerging. These
tests reveal that the Higgs boson discovered ten years ago
is remarkably consistent with the predictions of the theory
and provide stringent constraints on many models of new
phenomena beyond the standard model.},
Doi = {10.1038/s41586-022-04893-w},
Key = {fds376029}
}
@article{fds348468,
Author = {Kotwal, AV},
Title = {A fast method for particle tracking and triggering using
small-radius silicon detectors},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {957},
Pages = {6 pages},
Publisher = {Elsevier},
Year = {2020},
Month = {March},
url = {http://dx.doi.org/10.1016/j.nima.2020.163427},
Abstract = {We propose an algorithm, deployable on a highly-parallelized
graph computing architecture, to perform rapid
reconstruction of charged-particle trajectories in the high
energy collisions at the Large Hadron Collider and future
colliders. We use software emulation to show that the
algorithm can achieve an efficiency in excess of 99.95% for
reconstruction with good accuracy. The algorithm can be
implemented on silicon-based integrated circuits using
field-programmable gate array technology. Our approach can
enable a fast trigger for massive charged particles that
decay invisibly in the tracking volume, as in some
new-physics scenarios related to particulate dark matter. If
production of dark matter or other new neutral particles is
mediated by metastable charged particles and is not
associated with other triggerable energy deposition in the
detectors, our method would be useful for triggering on the
charged mediators using the small-radius silicon
detectors.},
Doi = {10.1016/j.nima.2020.163427},
Key = {fds348468}
}
@article{fds327183,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {A measurement of material in the ATLAS tracker using
secondary hadronic interactions in 7TeV pp
collisions},
Journal = {Journal of Instrumentation},
Volume = {11},
Number = {11},
Pages = {P11020-P11020},
Publisher = {IOP Publishing},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1088/1748-0221/11/11/P11020},
Abstract = {Knowledge of the material in the ATLAS inner tracking
detector is crucial in understanding the reconstruction of
charged-particle tracks, the performance of algorithms that
identify jets containing b-hadrons and is also essential to
reduce background in searches for exotic particles that can
decay within the inner detector volume. Interactions of
primary hadrons produced in pp collisions with the material
in the inner detector are used to map the location and
amount of this material. The hadronic interactions of
primary particles may result in secondary vertices, which in
this analysis are reconstructed by an inclusive
vertex-finding algorithm. Data were collected using
minimum-bias triggers by the ATLAS detector operating at the
LHC during 2010 at centre-of-mass energy √s = 7TeV, and
correspond to an integrated luminosity of 19nb-1. Kinematic
properties of these secondary vertices are used to study the
validity of the modelling of hadronic interactions in
simulation. Secondary-vertex yields are compared between
data and simulation over a volume of about 0.7 m3 around the
interaction point, and agreement is found within overall
uncertainties.},
Doi = {10.1088/1748-0221/11/11/P11020},
Key = {fds327183}
}
@article{fds347490,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker,
C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard,
J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL},
Title = {A measurement of the calorimeter response to single hadrons
and determination of the jet energy scale uncertainty using
LHC Run-1 pp-collision data with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {1},
Pages = {26},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4580-0},
Abstract = {A measurement of the calorimeter response to isolated
charged hadrons in the ATLAS detector at the LHC is
presented. This measurement is performed with
3.2 nb[Formula: see text] of proton-proton collision data
at [Formula: see text] [Formula: see text] from 2010 and
0.1 nb[Formula: see text] of data at [Formula: see
text] [Formula: see text] from 2012. A number of aspects of
the calorimeter response to isolated hadrons are explored.
After accounting for energy deposited by neutral particles,
there is a 5% discrepancy in the modelling, using various
sets of Geant4 hadronic physics models, of the calorimeter
response to isolated charged hadrons in the central
calorimeter region. The description of the response to
anti-protons at low momenta is found to be improved with
respect to previous analyses. The electromagnetic and
hadronic calorimeters are also examined separately, and the
detector simulation is found to describe the response in the
hadronic calorimeter well. The jet energy scale uncertainty
and correlations in scale between jets of different momenta
and pseudorapidity are derived based on these studies. The
uncertainty is 2-5% for jets with transverse momenta above
2 [Formula: see text], where this method provides the jet
energy scale uncertainty for ATLAS.},
Doi = {10.1140/epjc/s10052-016-4580-0},
Key = {fds347490}
}
@article{fds310391,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, MF and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {A measurement of the ratio of the production cross sections
for [Formula: see text] and [Formula: see text] bosons in
association with jets with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {12},
Pages = {3168},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3168-9},
Abstract = {The ratio of the production cross sections for [Formula: see
text] and [Formula: see text] bosons in association with
jets has been measured in proton-proton collisions at
[Formula: see text] with the ATLAS experiment at the Large
Hadron Collider. The measurement is based on the entire 2011
dataset, corresponding to an integrated luminosity of
[Formula: see text]. Inclusive and differential
cross-section ratios for massive vector bosons decaying to
electrons and muons are measured in association with jets
with transverse momentum [Formula: see text] and jet
rapidity [Formula: see text]. The measurements are compared
to next-to-leading-order perturbative QCD calculations and
to predictions from different Monte Carlo generators
implementing leading-order matrix elements supplemented by
parton showers.},
Doi = {10.1140/epjc/s10052-014-3168-9},
Key = {fds310391}
}
@article{fds307753,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {A measurement of the ratio of the W and Z cross sections
with exactly one associated jet in pp collisions at s=7TeV
with ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {708},
Number = {3-5},
Pages = {221-240},
Publisher = {Elsevier BV},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2012.01.042},
Abstract = {The ratio of production cross sections of the W and Z bosons
with exactly one associated jet is presented as a function
of jet transverse momentum threshold. The measurement has
been designed to maximise cancellation of experimental and
theoretical uncertainties, and is reported both within a
particle-level kinematic range corresponding to the detector
acceptance and as a total cross-section ratio. Results are
obtained with the ATLAS detector at the LHC in pp collisions
at a centre-of-mass energy of 7 TeV using an integrated
luminosity of 33 pb-1. The results are compared with
perturbative leading-order, leading-log, and
next-to-leading-order QCD predictions, and are found to
agree within experimental and theoretical uncertainties. The
ratio is measured for events with a single jet with pT>30
GeV to be 8.73±0.30(stat)±0.40(syst) in the electron
channel, and 8.49±0.23(stat)±0.33(syst) in the muon
channel. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.01.042},
Key = {fds307753}
}
@booklet{Abbott98j,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del-Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di-Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {A measurement of the W Boson mass at the fermilab pp¯
Collider},
Journal = {Physical Review Letters},
Volume = {80},
Number = {14},
Pages = {3008-3013},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.3008},
Abstract = {We report a measurement of the W boson mass based on an
integrated luminosity of 82pb-1 from pp¯ collisions at √s
= 1.8 TeV recorded in 1994-1995 by the D0 detector at the
Fermilab Tevatron. We identify W bosons by their decays to
ev and extract the mass by fitting the transverse mass
spectrum from 28 323 W boson candidates. A sample of 3563
dielectron events, mostly due to Z → ee decays, constrains
models of W boson production and the detector. We measure MW
= 80.44 ± 0.10(stat) ± 0.07(syst) GeV. By combining this
measurement with our result form the 1992-1993 data set, we
obtain MW = 80.43 ± 0.11 GeV. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.80.3008},
Key = {Abbott98j}
}
@article{fds310358,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyka, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa,
C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araquea, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
M and Armbruster, AJ and Arnaez, O and Arnal, V},
Title = {A neural network clustering algorithm for the ATLAS silicon
pixel detector},
Journal = {Journal of Instrumentation},
Volume = {9},
Number = {9},
Pages = {P09009-P09009},
Publisher = {IOP Publishing},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1088/1748-0221/9/09/P09009},
Abstract = {A novel technique to identify and split clusters created by
multiple charged particles in the ATLAS pixel detector using
a set of artificial neural networks is presented. Such
merged clusters are a common feature of tracks originating
from highly energetic objects, such as jets. Neural networks
are trained using Monte Carlo samples produced with a
detailed detector simulation. This technique replaces the
former clustering approach based on a connected component
analysis and charge interpolation. The performance of the
neural network splitting technique is quantified using data
from proton-proton collisions at the LHC collected by the
ATLAS detector in 2011 and from Monte Carlo simulations.
This technique reduces the number of clusters shared between
tracks in highly energetic jets by up to a factor of three.
It also provides more precise position and error estimates
of the clusters in both the transverse and longitudinal
impact parameter resolution.},
Doi = {10.1088/1748-0221/9/09/P09009},
Key = {fds310358}
}
@article{fds315918,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {A new method to distinguish hadronically decaying boosted
Z bosons from W bosons using the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {238},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4065-1},
Abstract = {The distribution of particles inside hadronic jets produced
in the decay of boosted <i>W</i> and <i>Z</i> bosons can be
used to discriminate such jets from the continuum
background. Given that a jet has been identified as likely
resulting from the hadronic decay of a boosted <i>W</i> or
<i>Z</i> boson, this paper presents a technique for further
differentiating <i>Z</i> bosons from <i>W</i> bosons. The
variables used are jet mass, jet charge, and a
<i>b</i>-tagging discriminant. A likelihood tagger is
constructed from these variables and tested in the
simulation of [Formula: see text] for bosons in the
transverse momentum range 200 GeV [Formula: see
text] 400 GeV in [Formula: see text] TeV <i>pp</i>
collisions with the ATLAS detector at the LHC. For
<i>Z</i>-boson tagging efficiencies of [Formula: see text],
50, and [Formula: see text], one can achieve [Formula: see
text]-boson tagging rejection factors ([Formula: see text])
of 1.7, 8.3 and 1000, respectively. It is not possible to
measure these efficiencies in the data due to the lack of a
pure sample of high [Formula: see text], hadronically
decaying <i>Z</i> bosons. However, the modelling of the
tagger inputs for boosted <i>W</i> bosons is studied in data
using a [Formula: see text]-enriched sample of events in
20.3 fb[Formula: see text] of data at [Formula: see text]
TeV. The inputs are well modelled within uncertainties,
which builds confidence in the expected tagger
performance.},
Doi = {10.1140/epjc/s10052-016-4065-1},
Key = {fds315918}
}
@article{fds313582,
Author = {ATLAS Collaboration},
Title = {A particle consistent with the Higgs boson observed with the
ATLAS detector at the Large Hadron Collider.},
Journal = {Science (New York, N.Y.)},
Volume = {338},
Number = {6114},
Pages = {1576-1582},
Publisher = {American Association for the Advancement of Science
(AAAS)},
Year = {2012},
Month = {December},
ISSN = {0036-8075},
url = {http://dx.doi.org/10.1126/science.1232005},
Abstract = {Nearly 50 years ago, theoretical physicists proposed that a
field permeates the universe and gives energy to the vacuum.
This field was required to explain why some, but not all,
fundamental particles have mass. Numerous precision
measurements during recent decades have provided indirect
support for the existence of this field, but one crucial
prediction of this theory has remained unconfirmed despite
30 years of experimental searches: the existence of a
massive particle, the standard model Higgs boson. The ATLAS
experiment at the Large Hadron Collider at CERN has now
observed the production of a new particle with a mass of 126
giga-electron volts and decay signatures consistent with
those expected for the Higgs particle. This result is strong
support for the standard model of particle physics,
including the presence of this vacuum field. The existence
and properties of the newly discovered particle may also
have consequences beyond the standard model
itself.},
Doi = {10.1126/science.1232005},
Key = {fds313582}
}
@article{fds225678,
Author = {A.V. Kotwal and T. Aaltonen et al (CDF Collaboration)},
Title = {A precise measurement of the W-boson mass with the Collider
Detector at Fermilab},
Journal = {Phys. Rev. D},
Volume = {89},
Number = {072003},
Year = {2014},
Month = {Spring},
Key = {fds225678}
}
@article{fds321115,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {A search for an excited muon decaying to a muon and two jets
in pp collisions at √ s = 8 TeV with the ATLAS
detector},
Journal = {New Journal of Physics},
Volume = {18},
Number = {7},
Pages = {073021-073021},
Publisher = {IOP Publishing},
Year = {2016},
Month = {July},
url = {http://dx.doi.org/10.1088/1367-2630/18/7/073021},
Abstract = {Anew search signature for excited leptons is explored.
Excited muons are sought in the channel pp → μμ∗→
μμ jet jet, assuming both the production and decay occur
via a contact interaction. The analysis is based on 20.3
fb-1 of pp collision data at a centre-of-mass energy of s =
8 TeV taken with the ATLAS detector at the large hadron
collider. No evidence of excited muons is found, and limits
are set at the 95% confidence level on the cross section
times branching ratio as a function of the excited-muonmass
μμ∗. For μμ∗between 1.3 and 3.0 TeV, the upper limit
on φB (μ∗→ μqq) is between 0.6 and 1 fb. Limits on sB
are converted to lower bounds on the compositeness scale. In
the limiting case L = μμ∗, excitedmuonswith amass
below2.8 TeVare excluded.With the samemodel assumptions,
these limits at larger μ∗masses improve upon previous
limits fromtraditional searches based on the gauge-mediated
decay μ∗→ μγ.},
Doi = {10.1088/1367-2630/18/7/073021},
Key = {fds321115}
}
@article{fds307687,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
A and Artoni, G},
Title = {A search for flavour changing neutral currents in top-quark
decays in pp collision data collected with the ATLAS
detector at √s = 7 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {9},
Pages = {1-36},
Publisher = {Springer Nature},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2012)139},
Abstract = {A search for flavour changing neutral current (FCNC)
processes in top-quark decays by the ATLAS Collaboration is
presented. Data collected from pp collisions at the LHC at a
centre-of-mass energy of √s = 7 TeV during 2011,
corresponding to an integrated luminosity of 2.1 fb-1, were
used. A search was performed for top-quark pair-production
events, with one top quark decaying through the t → Zq
FCNC (q = u, c) channel, and the other through the Standard
Model dominant mode t → Wb. Only the decays of the Z boson
to charged leptons and leptonic W-boson decays were
considered as signal. Consequently, the final-state topology
is characterised by the presence of three isolated charged
leptons, at least two jets and missing transverse momentum
from the undetected neutrino. No evidence for an FCNC signal
was found. An upper limit on the t → Zq branching ratio of
BR(t → Zq) < 0.73% is set at the 95% confidence level.
Copyright CERN.},
Doi = {10.1007/JHEP09(2012)139},
Key = {fds307687}
}
@article{fds307624,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, R and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, R and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Gimenez, VC and Castro,
NF and Cataldi, G and Catastini, R and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, R and Citron, ZH and Citterio, M and Ciubancan, M and Clark,
A},
Title = {A search for high-mass resonances decaying to
τ+τ- in pp collisions at
√s=7 TeV with the ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {719},
Number = {4-5},
Pages = {242-260},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.040},
Abstract = {© 2012 CERN This Letter presents a search for high-mass
resonances decaying into τ+τ− final states using
proton-proton collisions at s=7 TeV produced by the Large
Hadron Collider. The data were recorded with the ATLAS
detector and correspond to an integrated luminosity of 4.6
fb−1. No statistically significant excess above the
Standard Model expectation is observed; 95% credibility
upper limits are set on the cross section times branching
fraction of Z′ resonances decaying into τ+τ− pairs as
a function of the resonance mass. As a result, Z′ bosons
of the Sequential Standard Model with masses less than 1.40
TeV are excluded at 95% credibility.},
Doi = {10.1016/j.physletb.2013.01.040},
Key = {fds307624}
}
@article{fds310274,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {A search for high-mass resonances decaying to
τ+τ− in pp collisions at √s =8
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {7},
Publisher = {Springer Nature},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2015)157},
Abstract = {Abstract: A search for high-mass resonances decaying into
τ+τ− final states using proton-proton collisions at
s=8$$ \sqrt{s}=8 $$ TeV produced by the Large Hadron
Collider is presented. The data were recorded with the ATLAS
detector and correspond to an integrated luminosity of
19.5–20.3 fb−1. No statistically significant excess
above the Standard Model expectation is observed; 95%
credibility upper limits are set on the cross section times
branching fraction of Z′ resonances decaying into τ+τ−
pairs as a function of the resonance mass. As a result, Z′
bosons of the Sequential Standard Model with masses less
than 2.02 TeV are excluded at 95% credibility. The impact of
the fermionic couplings on the Z′ acceptance is
investigated and limits are also placed on a Z′ model that
exhibits enhanced couplings to third-generation
fermions.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP07(2015)157},
Key = {fds310274}
}
@article{fds347474,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
Title = {A search for pair-produced resonances in four-jet final
states at s = 13 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {3},
Pages = {250},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5693-4},
Abstract = {A search for massive coloured resonances which are
pair-produced and decay into two jets is presented. The
analysis uses 36.7 fb - 1 of s = 13 TeV <i>pp</i> collision
data recorded by the ATLAS experiment at the LHC in 2015 and
2016. No significant deviation from the background
prediction is observed. Results are interpreted in a SUSY
simplified model where the lightest supersymmetric particle
is the top squark, t ~ , which decays promptly into two
quarks through <i>R</i>-parity-violating couplings. Top
squarks with masses in the range 100 GeV < m t ~ < 410
GeV are excluded at 95% confidence level. If the decay is
into a <i>b</i>-quark and a light quark, a dedicated
selection requiring two <i>b</i>-tags is used to exclude
masses in the ranges 100 GeV < m t ~ < 470 GeV and 480
GeV < m t ~ < 610 GeV . Additional limits are set on the
pair-production of massive colour-octet resonances.},
Doi = {10.1140/epjc/s10052-018-5693-4},
Key = {fds347474}
}
@article{fds307625,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung,
C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker,
S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, E and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
J},
Title = {A search for prompt lepton-jets in pp collisions at
√s=7 TeV with the ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {719},
Number = {4-5},
Pages = {299-317},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.034},
Abstract = {© 2013 CERN We present a search for a light (mass <2GeV)
boson predicted by Hidden Valley supersymmetric models that
decays into a final state consisting of collimated muons or
electrons, denoted “lepton-jets”. The analysis uses
5fb−1 of s=7TeV proton–proton collision data recorded by
the ATLAS detector at the Large Hadron Collider to search
for the following signatures: single lepton-jets with at
least four muons; pairs of lepton-jets, each with two or
more muons; and pairs of lepton-jets with two or more
electrons. This study finds no statistically significant
deviation from the Standard Model prediction and places 95%
confidence-level exclusion limits on the production cross
section times branching ratio of light bosons for several
parameter sets of a Hidden Valley model.},
Doi = {10.1016/j.physletb.2013.01.034},
Key = {fds307625}
}
@article{fds356783,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {A search for prompt lepton-jets in pp collisions at √s = 8
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {2},
Pages = {1-51},
Year = {2016},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2016)062},
Abstract = {Abstract: A search is presented for a new, light boson with
a mass of about 1 GeV and decaying promptly to jets of
collimated electrons and/or muons (lepton-jets). The
analysis is performed with 20.3 fb−1 of data collected by
the ATLAS detector at the Large Hadron Collider in
proton-proton collisions at a centre-of-mass energy of 8
TeV. Events are required to contain at least two
lepton-jets. This study finds no statistically significant
deviation from predictions of the Standard Model and places
95% confidence-level upper limits on the contribution of new
phenomena beyond the SM, incuding SUSY-portal and
Higgs-portal models, on the number of events with
lepton-jets.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP02(2016)062},
Key = {fds356783}
}
@article{fds356688,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {A search for resonances decaying into a Higgs boson and a
new particle X in the XH → qqbb final state with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {779},
Pages = {24-45},
Year = {2018},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2018.01.042},
Abstract = {A search for heavy resonances decaying into a Higgs boson
(H) and a new particle (X) is reported, utilizing 36.1
fb−1 of proton–proton collision data at s=13TeV
collected during 2015 and 2016 with the ATLAS detector at
the CERN Large Hadron Collider. The particle X is assumed to
decay to a pair of light quarks, and the fully hadronic
final state XH→qq¯′bb¯ is analysed. The search
considers the regime of high XH resonance masses, where the
X and H bosons are both highly Lorentz-boosted and are each
reconstructed using a single jet with large radius
parameter. A two-dimensional phase space of XH mass versus X
mass is scanned for evidence of a signal, over a range of XH
resonance mass values between 1 TeV and 4 TeV, and for X
particles with masses from 50 GeV to 1000 GeV. All search
results are consistent with the expectations for the
background due to Standard Model processes, and 95% CL upper
limits are set, as a function of XH and X masses, on the
production cross-section of the XH→qq¯′bb¯
resonance.},
Doi = {10.1016/j.physletb.2018.01.042},
Key = {fds356688}
}
@article{fds308097,
Author = {Abulencia, and A, and others},
Title = {A search for scalar bottom quarks from gluino decays in
$\bar{p}p$ collisions at $\sqrt{s} =$ 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {17},
Pages = {171802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.171802},
Abstract = {We searched for scalar bottom quarks in 156 pb-1 of p anti-p
collisions at s**(1/2) = 1.96 TeV recorded by the CDF II
experiment at the Tevatron. Scalar bottom quarks can be
produced from gluino decays in R-parity conserving models of
supersymmetry when the mass of the gluino exceeds that of
the scalar bottom quark. Then, a scalar bottom quark. Then,
a scalar bottom quark can decay into a bottom quark and a
neutralino. To search for this scenario, we investigated
events with large missing transverse energy and at least
three jets, two or more of which were identified as
containing a secondary vertex from the hadronization of b
quarks. We found four candidate events, where 2.6 +/- 0.7
are expected from standard model processes, and placed 95\%
confidence level lower limits on gluino and scalar bottom
quark masses of up to 280 and 240 GeV/c2,
respectively.},
Doi = {10.1103/physrevlett.96.171802},
Key = {fds308097}
}
@article{fds308110,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH},
Title = {A search for t → τ ν q in t over(t, ̄)
production},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {639},
Number = {3-4},
Pages = {172-178},
Publisher = {Elsevier BV},
Year = {2006},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2006.06.030},
Abstract = {We present a search for t over(t, ̄) events with a tau
lepton in the final state. The data sample corresponds to an
integrated luminosity of 194 pb-1 collected with the CDF II
detector from p over(p, ̄) collisions at a center of mass
energy of 1.96 TeV. We observe two events with an expected
signal of 1.0 ± 0.2 events and a background of 1.3 ± 0.3
events. We determine a 95% confidence level upper limit on
rτ, the ratio of the measured rate of t → τ ν q to the
expectation, of 5.2. © 2006 Elsevier B.V. All rights
reserved.},
Doi = {10.1016/j.physletb.2006.06.030},
Key = {fds308110}
}
@article{fds366276,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {A search for the decays of stopped long-lived particles at
√s = 13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2021)173},
Abstract = {A search for long-lived particles, which have come to rest
within the ATLAS detector, is presented. The subsequent
decays of these particles can produce high-momentum jets,
resulting in large out-of-time energy deposits in the ATLAS
calorimeters. These de- cays are detected using data
collected during periods in the LHC bunch structure when
collisions are absent. The analysed dataset is composed of
events from proton-proton collisions produced by the Large
Hadron Collider at a centre-of-mass energy of s = 13 TeV and
recorded by the ATLAS experiment during 2017 and 2018. The
dataset used for this search corresponds to a total live
time of 579 hours. The results of this search are used to
derive lower limits on the mass of gluino R-hadrons,
assuming a branching fraction B(g~→qq¯χ10) = 100%, with
masses of up to 1.4 TeV excluded for gluino lifetimes of
10−5 to 103 s. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP07(2021)173},
Key = {fds366276}
}
@article{fds307941,
Author = {al, AVKWTAE and Collaboration, CDF},
Title = {A Search for the Higgs Boson Produced in Association with
Z-> l+ l- Using the Matrix Element Method at CDF
II},
Journal = {Physical Review D},
Volume = {80},
Number = {071101 (R)},
Pages = {8},
Year = {2009},
Month = {Fall},
Key = {fds307941}
}
@article{fds307905,
Author = {Aaltonen, and T, and others},
Title = {A Search for the Higgs Boson Using Neural Networks in Events
with Missing Energy and $b$-quark Jets in $p\bar p$
Collisions at $\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {14},
Pages = {141801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.141801},
Abstract = {http://arxiv.org/abs/0911.3935},
Doi = {10.1103/PhysRevLett.104.141801},
Key = {fds307905}
}
@article{fds352891,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {A search for the Zγ decay mode of the Higgs boson in pp
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {809},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2020.135754},
Abstract = {A search for the Zγ decay of the Higgs boson, with Z boson
decays into pairs of electrons or muons is presented. The
analysis uses proton–proton collision data at s = 13 TeV
corresponding to an integrated luminosity of 139 fb−1
recorded by the ATLAS detector at the Large Hadron Collider.
The observed data are consistent with the expected
background with a p-value of 1.3%. An upper limit at 95%
confidence level on the production cross-section times the
branching ratio for pp→H→Zγ is set at 3.6 times the
Standard Model prediction while 2.6 times is expected in the
presence of the Standard Model Higgs boson. The best-fit
value for the signal yield normalised to the Standard Model
prediction is 2.0−0.9+1.0 where the statistical component
of the uncertainty is dominant.},
Doi = {10.1016/j.physletb.2020.135754},
Key = {fds352891}
}
@article{fds321123,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {A search for top squarks with R-parity-violating decays to
all-hadronic final states with the ATLAS detector in √s =
8 TeV proton-proton collisions},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {6},
Pages = {1-49},
Publisher = {Springer Nature},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2016)067},
Abstract = {A search for the pair production of top squarks, each with
R-parity-violating decays into two Standard Model quarks, is
performed using 17.4 fb−1 of √s = 8 TeV proton-proton
collision data recorded by the ATLAS experiment at the LHC.
Each top squark is assumed to decay to a b- and an s-quark,
leading to four quarks in the final state. Background
discrimination is achieved with the use of b-tagging and
selections on the mass and substructure of large-radius
jets, providing sensitivity to top squark masses as low as
100 GeV. No evidence of an excess beyond the Standard Model
background prediction is observed and top squarks decaying
to b¯ s¯ are excluded for top squark masses in the range
100 ≤ mt≤ 315 GeV at 95% confidence level.},
Doi = {10.1007/JHEP06(2016)067},
Key = {fds321123}
}
@article{fds315360,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {A search for tt resonances using lepton-plus-jets events in
proton-proton collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2015)148},
Abstract = {Abstract: A search for new particles that decay into top
quark pairs is reported. The search is performed with the
ATLAS experiment at the LHC using an integrated luminosity
of 20.3 fb−1 of proton-proton collision data collected at
a centre-of-mass energy of √s=8 TeV. The lepton-plus-jets
final state is used, where the top pair decays to
W+bW−b¯, with one W boson decaying leptonically and the
other hadronically. The invariant mass spectrum of top quark
pairs is examined for local excesses or deficits that are
inconsistent with the Standard Model predictions. No
evidence for a top quark pair resonance is found, and 95%
confidence-level limits on the production rate are
determined for massive states in benchmark models. The upper
limits on the cross-section times branching ratio of a
narrow Z′ boson decaying to top pairs range from 4.2 pb to
0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A
narrow leptophobic topcolour Z′ boson with mass below 1.8
TeV is excluded. Upper limits are set on the cross-section
times branching ratio for a broad colour-octet resonance
with Γ/m = 15% decaying to tt¯. These range from 4.8 pb to
0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein
excitation of the gluon in a Randall-Sundrum model is
excluded for masses below 2.2 TeV.},
Doi = {10.1007/JHEP08(2015)148},
Key = {fds315360}
}
@article{fds307784,
Author = {ATLAS Collaboration},
Title = {A search for ttbar resonances with the ATLAS detector in
2.05 fb^-1 of proton-proton collisions at sqrt(s) = 7
TeV},
Journal = {The European Physical Journal C},
Volume = {72},
Number = {7},
Pages = {2083},
Year = {2012},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2083-1},
Abstract = {A search for top quark pair resonances in final states
containing at least one electron or muon has been performed
with the ATLAS experiment at the CERN Large Hadron Collider.
The search uses a data sample corresponding to an integrated
luminosity of 2.05 fb<sup>-1</sup>, which was recorded in
2011 at a proton-proton centre-of-mass energy of 7 TeV. No
evidence for a resonance is found and limits are set on the
production cross-section times branching ratio to [Formula:
see text] for narrow and wide resonances. For narrow
<i>Z</i>' bosons, the observed 95 % Bayesian credibility
level limits range from 9.3 pb to 0.95 pb for masses in
the range of <i>m</i><sub><i>Z</i>'</sub>=500 GeV to
<i>m</i><sub><i>Z</i>'</sub>=1300 GeV. The corresponding
excluded mass region for a leptophobic topcolour <i>Z</i>'
boson (Kaluza-Klein gluon excitation in the Randall-Sundrum
model) is <i>m</i><sub><i>Z</i>'</sub><880 GeV ([Formula:
see text]).},
Doi = {10.1140/epjc/s10052-012-2083-1},
Key = {fds307784}
}
@article{fds212566,
Author = {A.V. Kotwal and ATLAS Collaboration},
Title = {A search for ttbar resonances with the ATLAS detector in
2.05/fb of proton-proton collisions at √s=7
TeV},
Journal = {Eur. Phys. J. C},
Volume = {72},
Pages = {2083},
Year = {2012},
Month = {July},
Key = {fds212566}
}
@article{fds307721,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {A search for tt̄ resonances in lepton+jets events with
highly boosted top quarks collected in pp collisions at √s
= 7TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {9},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP09(2012)041},
Abstract = {A search for resonant production of high-mass top-quark
pairs is performed on 2.05 fb-1 of proton-proton collisions
at √s = 7 TeV collected in 2011 with the ATLAS experiment
at the Large Hadron Collider. This analysis of the
lepton+jets final state is specifically designed for the
particular topology that arises from the decay of highly
boosted top quarks. The observed tt̄ invariant mass
spectrum is found to be compatible with the Standard Model
prediction and 95% credibility level upper limits are
derived on the tt̄ production rate through new massive
states. An upper limit of 0.7 pb is set on the production
cross section times branching fraction of a narrow 1 TeV
resonance. A Kaluza-Klein gluon with a mass smaller than 1.5
TeV is excluded.},
Doi = {10.1007/JHEP09(2012)041},
Key = {fds307721}
}
@article{fds356626,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {A strategy for a general search for new phenomena using
data-derived signal regions and its application within the
ATLAS experiment},
Journal = {European Physical Journal C},
Volume = {79},
Number = {2},
Year = {2019},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6540-y},
Abstract = {This paper describes a strategy for a general search used by
the ATLAS Collaboration to find potential indications of new
physics. Events are classified according to their final
state into many event classes. For each event class an
automated search algorithm tests whether the data are
compatible with the Monte Carlo simulated expectation in
several distributions sensitive to the effects of new
physics. The significance of a deviation is quantified using
pseudo-experiments. A data selection with a significant
deviation defines a signal region for a dedicated follow-up
analysis with an improved background expectation. The
analysis of the data-derived signal regions on a new dataset
allows a statistical interpretation without the large
look-elsewhere effect. The sensitivity of the approach is
discussed using Standard Model processes and benchmark
signals of new physics. As an example, results are shown for
3.2 fb- 1 of proton–proton collision data at a
centre-of-mass energy of 13 TeV collected with the ATLAS
detector at the LHC in 2015, in which more than 700 event
classes and more than 10 5 regions have been analysed. No
significant deviations are found and consequently no
data-derived signal regions for a follow-up analysis have
been defined.},
Doi = {10.1140/epjc/s10052-019-6540-y},
Key = {fds356626}
}
@article{fds346178,
Author = {Kotwal, J and Singh, V and Kotwal, A and Dutta, V and Nair,
V},
Title = {A study of haematological and bone marrow changes in
symptomatic patients with human immune deficiency virus
infection with special mention of functional iron
deficiency, anaemia of critically ill and haemophagocytic
lymphohistiocytosis.},
Journal = {Medical journal, Armed Forces India},
Volume = {69},
Number = {4},
Pages = {319-325},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.11.002},
Abstract = {<h4>Background</h4>Haematological abnormalities are among
the most common complications of HIV. These involve all
lineages of blood cells. Bone marrow studies form integral
part of complete workup of the HIV positive patients
specially when they present as case of pyrexia of unknown
origin (PUO), refractory anaemia and pancytopenia.<h4>Method</h4>55
HIV infected symptomatic patient requiring bone marrow
examination were included in the study. Relevant clinical
history, baseline haematological investigations including
full blood count, CD4 cell counts using flow cytometry were
recorded.<h4>Results</h4>Median ANC values in males were
found to be significantly lower than females (p = 0.046).
CD4 cell count statistically significantly correlated with
age, TLC, ANC & platelet count. Anaemia was present in 45
patients and out of which 66.66% patients had normocytic
normochromic anaemia. Iron deficiency anaemia was present in
(37.77%) patients and anaemia of chronic disease in (62.22%)
patients. 2 patients had anaemia of the critically ill. Two
patients had non-Hodgkin's lymphoma (NHL) and showed
lymphoma deposit in the bone marrow. Gelatinous degeneration
was seen in 3 patients. Ill formed epithelioid cell
granulomas were seen in 7 cases, and 2 cases were positive
for acid fast bacilli (AFB). Haemophagocytosis was seen in 8
cases; two cases later diagnosed as a case of infection
induced HLH. Leishmania donovani (LD) bodies seen in 2
cases.<h4>Conclusions</h4>Bone marrow study is an important
investigation in HIV infected symptomatic patients with
peripheral haematological abnormalities.},
Doi = {10.1016/j.mjafi.2012.11.002},
Key = {fds346178}
}
@article{fds346170,
Author = {Kotwal, A and Singh, H and Verma, AK and Gupta, RM and Jain, S and Sinha,
S and Joshi, RK and Teli, P and Khunga, V and Bhatnagar, A and Ranjan,
R},
Title = {A study of Hepatitis A and E virus seropositivity profile
amongst young healthy adults in India.},
Journal = {Medical journal, Armed Forces India},
Volume = {70},
Number = {3},
Pages = {225-229},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1016/j.mjafi.2014.06.016},
Abstract = {<h4>Background</h4>Various Serosurveys and studies provide
ample evidence of differing perspectives regarding
epidemiology of HAV and HEV in India. This study was
conducted to assess the seroprevalence of HAV and HEV and
its associated factors with an aim to provide inputs to
planners regarding requirement of HAV vaccine.<h4>Methods</h4>A
multi-centric cross sectional survey amongst 4175 healthy
trainees (young adults) was carried out in training centres,
selected by multistage random sampling, giving equal
representation to all regions of India. Sample size was
calculated by taking prevalence of HAV seropositivity
amongst adults as 60% and alpha 0.05.<h4>Results</h4>Seroprevalence
for HAV and HEV was 92.68% (95% CI 91.82, 93.47) and 17.05%
(15.90, 18.26), respectively. Logistic regression showed
that hand washing without soap, regular close contact with
domestic animals, consumption of unpasteurized milk and
regular consumption of food outside home were risk factors
for HAV (p < 0.05). For HEV, irregular hand washing,
consumption of unpasteurized milk and irregular consumption
of freshly prepared food were risk factors
(p < 0.05).<h4>Conclusion</h4>High level of immunity
against HAV among the healthy young adults clearly
demonstrates that vaccination against HAV is not required at
present in our country. The large proportion being
susceptible to HEV points towards the requirement of
preventive strategies in the form of safe drinking water
supply, hygiene, sanitation, increasing awareness and
behaviour change with respect to personal hygiene especially
hand and food hygiene.},
Doi = {10.1016/j.mjafi.2014.06.016},
Key = {fds346170}
}
@article{fds307928,
Author = {Aaltonen, and T, and others},
Title = {A study of the associated production of photons and
$b$-quark jets in $p \bar{p}$ collisions at $\sqrt{s} =
1.96$ TeV},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {5},
Pages = {052006},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.052006},
Abstract = {http://arxiv.org/abs/0912.3453},
Doi = {10.1103/PhysRevD.81.052006},
Key = {fds307928}
}
@article{fds307762,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {A study of the material in the ATLAS inner detector using
secondary hadronic interactions},
Journal = {Journal of Instrumentation},
Volume = {7},
Number = {1},
Pages = {P01013-P01013},
Publisher = {IOP Publishing},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/7/01/P01013},
Abstract = {The ATLAS inner detector is used to reconstruct secondary
vertices due to hadronic interactions of primary collision
products, so probing the location and amount of material in
the inner region of ATLAS. Data collected in 7 TeV pp
collisions at the LHC, with a minimum bias trigger, are used
for comparisons with simulated events. The reconstructed
secondary vertices have spatial resolutions ranging from ∼
200μm to 1 mm. The overall material description in the
simulation is validated to within an experimental
uncertainty of about 7%. This will lead to a better
understanding of the reconstruction of various objects such
as tracks, leptons, jets, and missing transverse momentum.
© 2012 CERN.},
Doi = {10.1088/1748-0221/7/01/P01013},
Key = {fds307762}
}
@article{fds346189,
Author = {Seth, T and Kotwal, A and Thakur, RK and Ganguly,
KK},
Title = {A study on community perceptions of common cancers,
determinants of community behaviour and program
implementation in New Delhi, India.},
Journal = {Asian Pacific journal of cancer prevention :
APJCP},
Volume = {13},
Number = {6},
Pages = {2781-2789},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.7314/apjcp.2012.13.6.2781},
Abstract = {Assessment of perceptions of the community, the determinants
and development of their behavior regarding common
malignancies, helps in establishing evidence-based
activities for prevention and early diagnosis of cancer.
However information on this important aspect is lacking in
our country. Qualitative methods were here used to obtain
information through in depth interviews and Focus Group
Discussions (FGDs) with all categories of identified
stakeholders. Most were unaware of the activities of the
cancer control program. Even the providers were not fully
conversant. All respondents mentioned lack of diagnostic and
treatment facilities in government, primary and secondary
level facilities. Perceptions of different categories of
stakeholders regarding why many community members did not
attend screening camps and other services reflect the
determinants of community behavior, acting independently as
well as in combination. The cancer control program was
thought to be restricted only to some private facilities and
overcrowded government tertiary care facilities where the
visits were time consuming. Almost all the facilities were
considered curative oriented. Issues of supervision,
monitoring and feedback were inadequately addressed by
providers who were inadequately trained in many program
activities. The program lacked effective planning,
coordination and appropriate implementation at the grass
roots level in Delhi. Social mobilization was grossly
inadequate, as most of the community members were unaware of
the existence of the program. Misconceptions about the risk
factors, signs and symptoms, diagnosis, and treatment were
common amongst community members as well as many of the
providers. Thus the national cancer control program in our
country needs further community participation and social
mobilization. Accessibility, availability, acceptability and
affordability of various preventive, curative and
rehabilitative activities, as well as intersectoral
coordination, training, supervision and monitoring of
program activities, all need to be addressed to ensure the
success of this important public health program.},
Doi = {10.7314/apjcp.2012.13.6.2781},
Key = {fds346189}
}
@article{fds347534,
Author = {Goel, N and Khandelwal, V and Pandya, K and Kotwal,
A},
Title = {Alcohol and Tobacco Use Among Undergraduate and Postgraduate
Medical Students in India: A Multicentric Cross-sectional
Study.},
Journal = {Central Asian journal of global health},
Volume = {4},
Number = {1},
Pages = {187},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.5195/cajgh.2015.187},
Abstract = {<h4>Background</h4>Substance use among medical fraternity is
a well-known phenomenon among both undergraduate (UG) and
postgraduate (PG) medical students. Yet, there have been
very few multi-centric studies to estimate the actual burden
of this problem in this important population group in India.
This study was conducted to estimate the prevalence of
alcohol and tobacco use, assess the knowledge and attitudes
towards this issue, and identify factors associated with
substance use among UG and PG medical students in
India.<h4>Methods</h4>A pre-tested, self-report, anonymous
questionnaire was administered to medical undergraduates and
post graduate medical residents of eight medical colleges
across India. This study used a convenience sample of
medical colleges with random selection of study participants
within each college for each group, UG and
PG.<h4>Results</h4>Prevalence of alcohol and tobacco use
among UG students was 16.6%, 95% CI [14.5, 18.9] and 8.0%,
95% CI [6.4, 9.6], respectively, whereas prevalence was
31.5%, 95% CI [26.3, 37.0] and 14.5%, 95% CI [10.7, 18.9],
respectively for PGs. For both substances, males had a
higher prevalence of use compared to females in both groups
(<i>p</i> < 0.001). Positive family history of substance use
(<i>p</i> < 0.001 for both groups) and early age of
initiation (<i>p</i> = 0.011 for tobacco; <i>p</i> > 0.05
for alcohol) were associated with a greater difficulty to
quit the habit. Over 90% of study participants felt that
substance use adversely affected their skills and reported
not using substances prior to managing their
patients.<h4>Conclusions</h4>Since substance use is a
relatively common phenomenon among UG and PG medical
students in India, future prospective studies and
interventions are required to better understand the pattern
of substance use and reduce its prevalence.},
Doi = {10.5195/cajgh.2015.187},
Key = {fds347534}
}
@article{fds354613,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Alignment of the ATLAS Inner Detector in Run
2},
Journal = {European Physical Journal C},
Volume = {80},
Number = {12},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08700-6},
Abstract = {The performance of the ATLAS Inner Detector alignment has
been studied using pp collision data at s=13TeV collected by
the ATLAS experiment during Run 2 (2015–2018) of the Large
Hadron Collider (LHC). The goal of the detector alignment is
to determine the detector geometry as accurately as possible
and correct for time-dependent movements. The Inner Detector
alignment is based on the minimization of track-hit
residuals in a sequence of hierarchical levels, from global
mechanical assembly structures to local sensors. Subsequent
levels have increasing numbers of degrees of freedom; in
total there are almost 750,000. The alignment determines
detector geometry on both short and long timescales, where
short timescales describe movements within an LHC fill. The
performance and possible track parameter biases originating
from systematic detector deformations are evaluated.
Momentum biases are studied using resonances decaying to
muons or to electrons. The residual sagitta bias and
momentum scale bias after alignment are reduced to less than
∼0.1TeV-1 and 0.9 × 10 - 3, respectively. Impact
parameter biases are also evaluated using tracks within
jets.},
Doi = {10.1140/epjc/s10052-020-08700-6},
Key = {fds354613}
}
@article{fds347526,
Author = {Biswas, D and Kotwal, A and Kakati, B and Ahmad, S},
Title = {Amphotericin B Resistant Apophysomyces elegans Causing
Rhino-oculo-Cerebral Mucormycosis in an Immunocompetent
Host.},
Journal = {Journal of clinical and diagnostic research :
JCDR},
Volume = {9},
Number = {8},
Pages = {DD01-DD02},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.7860/jcdr/2015/13929.6272},
Abstract = {Mucormycosis, an angioinvasive infection is caused by the
ubiquitous filamentous fungi of the order Mucorales and
class Mucormycetes. Reports of this disease are on the rise
over the past few decades. Rhino-oculo-Cerebral presentation
associated with uncontrolled diabetes is the predominant
characteristic of this entity. We report here a case of
rhinooculocerebral mucormycosis (ROCM) due to Apophysomyces
elegans (A. elegans) in a 45-year-old diabetic lady with
background illness of hypothyroidism and
polyradiculoneuropathy. Though this condition is usually
managed with surgical debridement of the affected tissue and
medical therapy with Amphotericin B, the isolate recovered
in our case was found to be resistant to Amphotericin
B.},
Doi = {10.7860/jcdr/2015/13929.6272},
Key = {fds347526}
}
@article{fds346191,
Author = {Kotwal, A and Biswas, D and Sharma, JP and Gupta, A and Jindal,
P},
Title = {An observational study on the epidemiological and
mycological profile of Candidemia in ICU
patients.},
Journal = {Medical science monitor : international medical journal of
experimental and clinical research},
Volume = {17},
Number = {11},
Pages = {CR663-CR668},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.12659/msm.882053},
Abstract = {<h4>Background</h4>This study aimed to analyze the
epidemiological and mycological profile of candidemia in
intensive care unit (ICU) patients attending a tertiary care
teaching hospital in the Himalayan region of northern
India.<h4>Material/methods</h4>A 15-bed medico-surgical ICU
and a 5-bed pediatric ICU. Ninety-one consecutively admitted
ICU patients were screened for the presence of candidemia by
performing blood cultures at periodic intervals.<h4>Results</h4>The
recovered Candida isolates were speciated and subjected to
antifungal susceptibility testing using standard procedures.
Forty-one of the recruited patients (45%) were found to be
candidemic, with the majority of patients being in the
extremes of age (13 neonates and 15 >65 years of age). Four
risk factors were found to be significantly associated with
the occurrence of candidemia in our patients - a period of
hospitalization exceeding 7 days (p=0.0008), previous use of
antibiotics (p=0.001), presence of chronic renal failure
(p=0.003), and ongoing cancer chemotherapy (p= 0.041).
Ninety-six Candida isolates were recovered from the 41
culture-positive patients, with Candida albicans being the
commonest isolate recovered (n=75, 78.1%), followed by
Candida tropicalis (n=15, 16%), and Candida glabrata (n=6,
6.5%). Fluconazole resistance was observed among 26% of all
Candida isolates and 17.3% of C. albicans
isolates.<h4>Conclusions</h4>Contrary to the majority of
recent reports, species shift towards non-albicans
candidemia has not been observed in our center, though the
prevalence of azole resistance is alarmingly high even among
the C. albicans isolates.},
Doi = {10.12659/msm.882053},
Key = {fds346191}
}
@article{fds347528,
Author = {Sahai, K and Kotwal, A},
Title = {Anaemia prevention in the community: students as change
agents.},
Journal = {Medical education},
Volume = {49},
Number = {5},
Pages = {518-519},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1111/medu.12683},
Doi = {10.1111/medu.12683},
Key = {fds347528}
}
@article{fds308060,
Author = {Abulencia, and A, and others},
Title = {Analysis of the quantum numbers J(PC) of the
X(3872)},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {13},
Pages = {132002},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.132002},
Abstract = {We present an analysis of angular distributions and
correlations of the X(3872) particle in the exclusive decay
mode X(3872)-->J/psipi+pi- with J/psi-->µ+µ-. We use 780
pb-1 of data from p[overline p] collisions at sqrt(s)=1.96
TeV collected with the CDF II detector at the Fermilab
Tevatron. We derive constraints on spin, parity, and charge
conjugation parity of the X(3872) particle by comparing
measured angular distributions of the decay products with
predictions for different JPC hypotheses. The assignments
JPC=1++ and 2-+ are the only ones consistent with the
data.},
Doi = {10.1103/physrevlett.98.132002},
Key = {fds308060}
}
@article{fds356714,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Analysis of the Wtb vertex from the measurement of
triple-differential angular decay rates of single top quarks
produced in the t-channel at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {12},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2017)017},
Abstract = {The electroweak production and subsequent decay of single
top quarks in the t-channel is determined by the properties
of the Wtb vertex, which can be described by the complex
parameters of an effective Lagrangian. An analysis of a
triple-differential decay rate in t-channel production is
used to simultaneously determine five generalised helicity
fractions and phases, as well as the polarisation of the
produced top quark. The complex parameters are then
constrained. This analysis is based on 20.2 fb−1 of
proton-proton collision data at a centre-of-mass energy of 8
TeV collected with the ATLAS detector at the LHC. The
fraction of decays containing transversely polarised W
bosons is measured to be f1 = 0.30 ± 0.05. The phase
between amplitudes for transversely and longitudinally
polarised W bosons recoiling against left-handed b-quarks is
measured to be δ− = 0.002π+ 0.017π+ 0.016π, giving no
indication of CP violation. The fractions of longitudinal or
transverse W bosons accompanied by right-handed b-quarks are
also constrained. Based on these measurements, limits are
placed at 95% CL on the ratio of the complex coupling
parameters Re [gR/VL ∈ [−0.12, 0.17] and Im [gR/VL ∈
[−0.07, 0.06]. Constraints are also placed on the ratios
|VR/VL| and |gL/VL|. In addition, the polarisation of single
top quarks in the t-channel is constrained to be P > 0.72
(95% CL). None of the above measurements make assumptions
about the value of any of the other parameters or couplings
and all of them are in agreement with the Standard
Model.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP12(2017)017},
Key = {fds356714}
}
@article{fds356655,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
H},
Title = {Angular analysis of Bd0 → K
∗ μ + μ − decays in
pp collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {10},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2018)047},
Abstract = {An angular analysis of the decay Bd0 → K∗μ+μ− is
presented, based on proton-proton collision data recorded by
the ATLAS experiment at the LHC. The study is using 20.3
fb−1 of integrated luminosity collected during 2012 at
centre-of-mass energy of s=8 TeV. Measurements of the K*
longitudinal polarisation fraction and a set of angular
parameters obtained for this decay are presented. The
results are compatible with the Standard Model
predictions.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP10(2018)047},
Key = {fds356655}
}
@article{fds373908,
Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi,
G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori,
G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
Title = {Anomaly detection search for new resonances decaying into a
Higgs boson and a generic new particle X in hadronic final
states using Formula Presented pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {5},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.108.052009},
Abstract = {A search is presented for a heavy resonance Formula
Presented decaying into a Standard Model Higgs boson Formula
Presented and a new particle Formula Presented in a fully
hadronic final state. The full Large Hadron Collider run 2
dataset of proton-proton collisions at Formula Presented
collected by the ATLAS detector from 2015 to 2018 is used
and corresponds to an integrated luminosity of Formula
Presented. The search targets the high Formula
Presented-mass region, where the Formula Presented and
Formula Presented have a significant Lorentz boost in the
laboratory frame. A novel application of anomaly detection
is used to define a general signal region, where events are
selected solely because of their incompatibility with a
learned background-only model. It is constructed using a
jet-level tagger for signal-model-independent selection of
the boosted Formula Presented particle, representing the
first application of fully unsupervised machine learning to
an ATLAS analysis. Two additional signal regions are
implemented to target a benchmark Formula Presented decay
into two quarks, covering topologies where the Formula
Presented is reconstructed as either a single large-radius
jet or two small-radius jets. The analysis selects Higgs
boson decays into Formula Presented, and a dedicated
neural-network-based tagger provides sensitivity to the
boosted heavy-flavor topology. No significant excess of data
over the expected background is observed, and the results
are presented as upper limits on the production cross
section Formula Presented) for signals with Formula
Presented between 1.5 and 6 TeV and Formula Presented
between 65 and 3000 GeV.},
Doi = {10.1103/PhysRevD.108.052009},
Key = {fds373908}
}
@article{fds347535,
Author = {Bangalore, S and Toklu, B and Kotwal, A and Volodarskiy, A and Sharma,
S and Kirtane, AJ and Feit, F},
Title = {Anticoagulant therapy during primary percutaneous coronary
intervention for acute myocardial infarction: a
meta-analysis of randomized trials in the era of stents and
P2Y12 inhibitors.},
Journal = {BMJ (Clinical research ed.)},
Volume = {349},
Pages = {g6419},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1136/bmj.g6419},
Abstract = {<h4>Objectives</h4>To investigate the relative benefits of
unfractionated heparin, low molecular weight heparin(LMWH),
fondaparinux, and bivalirudin as treatment options for
patients with ST segment elevation myocardial infarction
undergoing percutaneous coronary intervention
(PCI).<h4>Design</h4>Mixed treatment comparison and direct
comparison meta-analysis of randomized trials in the era of
stents and P2Y12 inhibitors.<h4>Data sources and study
selection</h4>A search of Medline, Embase, Cochrane Central
Register of Controlled Trials (CENTRAL) for randomized
trials comparing unfractionated heparin plus glycoprotein
IIb/IIIa inhibitor(GpIIb/IIIa inhibitor), unfractionated
heparin, bivalirudin, fondaparinux, or LMWH plus GpIIb/IIIa
inhibitor for patients undergoing primary
PCI.<h4>Outcomes</h4>The primary efficacy outcome was short
term (in hospital or within 30 days) major adverse
cardiovascular event; the primary safety outcome was short
term major bleeding.<h4>Results</h4>We identified 22
randomized trials that enrolled 22,434 patients. In the
mixed treatment comparison models, when compared with
unfractionated heparin plus GpIIb/IIIa inhibitor,
unfractionated heparin was associated with a higher risk of
major adverse cardiovascular events (relative risk 1.49 (95%
confidence interval 1.21 to 1.84), as were bivalirudin
(relative risk 1.34 (1.01 to 1.78)) and fondaparinux (1.78
(1.01 to 3.14)). LMWH plus GpIIb/IIIa inhibitor showed
highest treatment efficacy, followed (in order) by
unfractionated heparin plus GpIIb/IIIa inhibitor,
bivalirudin, unfractionated heparin, and fondaparinux.
Bivalirudin was associated with lower major bleeding risk
compared with unfractionated heparin plus GpIIb/IIIa
inhibitor (relative risk 0.47 (0.30 to 0.74)) or
unfractionated heparin (0.58 (0.37 to 0.90)). Bivalirudin,
followed by unfractionated heparin, LMWH plus GpIIb/IIIa
inhibitor, unfractionated heparin plus GpIIb/IIIa inhibitor,
and fondaparinux were the hierarchy for treatment safety.
Results were similar in direct comparison meta-analyses:
bivalirudin was associated with a 39%, 44%, and 65% higher
risk of myocardial infarction, urgent revascularization, and
stent thrombosis respectively when compared with
unfractionated heparin with or without GpIIb/IIIa inhibitor.
However, bivalirudin was associated with a 48% lower risk of
major bleeding compared with unfractionated heparin plus
GpIIb/IIIa inhibitor and 32% lower compared with
unfractionated heparin alone.<h4>Conclusions</h4>In patients
undergoing primary PCI, unfractionated heparin plus
GpIIb/IIIa inhibitor and LMWH plus GpIIb/IIIa inhibitor were
most efficacious, with the lowest rate of major adverse
cardiovascular events, whereas bivalirudin was safest, with
the lowest bleeding. These relationships should be
considered in selecting anticoagulant therapies in patients
undergoing primary PCI.},
Doi = {10.1136/bmj.g6419},
Key = {fds347535}
}
@article{fds347529,
Author = {Nair, V and Sharma, D and Sahni, AK and Grover, N and Shankar, S and Jaiswal, SS and Dalal, SS and Basannar, DR and Phutane, VS and Kotwal,
A and Gopal Rao and G and Batura, D and Venkatesh, MD and Sinha, T and Kumar,
S and Joshi, DP},
Title = {Antimicrobial use and antimicrobial resistance in nosocomial
pathogens at a tertiary care hospital in
Pune.},
Journal = {Medical journal, Armed Forces India},
Volume = {71},
Number = {2},
Pages = {112-119},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1016/j.mjafi.2014.12.024},
Abstract = {<h4>Background</h4>Resistance to antimicrobial agents is
emerging in wide variety of nosocomial and community
acquired pathogens. Widespread and often inappropriate use
of broad spectrum antimicrobial agents is recognized as a
significant contributing factor to the development and
spread of bacterial resistance. This study was conducted to
gain insight into the prevalent antimicrobial prescribing
practices, and antimicrobial resistance pattern in
nosocomial pathogens at a tertiary care hospital in Pune,
India.<h4>Methods</h4>Series of one day cross sectional
point prevalence surveys were carried out on four days
between March and August 2014. All eligible in patients were
included in the study. A structured data entry form was used
to collect the data for each patient. Relevant samples were
collected for microbiological examination from all the
clinically identified hospital acquired infection
cases.<h4>Results</h4>41.73% of the eligible patients (95%
CI: 39.52-43.97) had been prescribed at least one
antimicrobial during their stay in the hospital.
Beta-lactams (38%) were the most prescribed antimicrobials,
followed by Protein synthesis inhibitors (24%). Majority of
the organisms isolated from Hospital acquired infection (HAI
cases) were found to be resistant to the commonly used
antimicrobials viz: Cefotaxime, Ceftriaxone, Amikacin,
Gentamicin and Monobactams.<h4>Conclusion</h4>There is need
to have regular antimicrobial susceptibility surveillance
and dissemination of this information to the clinicians. In
addition, emphasis on the rational use of antimicrobials,
antimicrobial rotation and strict adherence to the standard
treatment guidelines is very essential.},
Doi = {10.1016/j.mjafi.2014.12.024},
Key = {fds347529}
}
@article{fds346172,
Author = {Sarkar, P and Biswas, D and Sindhwani, G and Rawat, J and Kotwal, A and Kakati, B},
Title = {Application of lipoarabinomannan antigen in tuberculosis
diagnostics: current evidence.},
Journal = {Postgraduate medical journal},
Volume = {90},
Number = {1061},
Pages = {155-163},
Year = {2014},
Month = {March},
url = {http://dx.doi.org/10.1136/postgradmedj-2013-132053},
Abstract = {Tests based on the detection of mycobacterial
lipoarabinomannan (LAM) antigen in urine have emerged as
potential point-of-care tests for tuberculosis (TB). We
aimed to assimilate the current evidence regarding the
diagnostic performance of LAM assays and to ascertain their
clinical indication in settings with high and low prevalence
of HIV-TB co-infection. Owing to suboptimal sensitivity, the
urinary LAM assays are unsuitable as general screening tests
for TB. However, unlike traditional diagnostic methods, they
demonstrate improved sensitivity in HIV-TB co-infection
which further increases with low CD4 counts. Accordingly,
these assays are indicated as rule-in tests for TB in
patients with advanced HIV-induced immunosuppression, and
facilitate the early initiation of antituberculous treatment
in them. They also offer incremental sensitivity and
specificity when used as adjunct tests to smear microscopy
and chest radiography in HIV-TB co-infection. They obviate
the biohazards associated with sputum samples and provide an
alternative diagnostic tool in sputum-scarce patients.
Notwithstanding these advantages, the specificity of these
assays is variable, which is mostly attributable to
misclassification bias and cross-reactivity with
non-tuberculous mycobacteria or other commensal flora.
Furthermore, the inability to detect low titres of antigen
in HIV-uninfected patients makes these assays unsuitable for
use in settings with a low HIV prevalence. Future research
targeted towards inclusion of specific monoclonal antibodies
and more sensitive immunoassay platforms might help to
improve the diagnostic performance of these assays and
extend their applicability to the general population of
patients with TB.},
Doi = {10.1136/postgradmedj-2013-132053},
Key = {fds346172}
}
@article{fds347533,
Author = {Kotwal, A and Biswas, D and Kakati, B and Roy, S and Chauhan,
BS},
Title = {Aspergillus nidulans causing primary cutaneous aspergillosis
in an immunocompetent patient.},
Journal = {Cutis},
Volume = {95},
Number = {1},
Pages = {E1-E3},
Year = {2015},
Month = {January},
Key = {fds347533}
}
@article{fds356564,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira,
RA},
Title = {ATLAS b-jet identification performance and efficiency
measurement with tt¯ events in pp collisions at √s=13
TeV},
Journal = {European Physical Journal C},
Volume = {79},
Number = {11},
Year = {2019},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7450-8},
Abstract = {The algorithms used by the ATLAS Collaboration during Run 2
of the Large Hadron Collider to identify jets containing
b-hadrons are presented. The performance of the algorithms
is evaluated in the simulation and the efficiency with which
these algorithms identify jets containing b-hadrons is
measured in collision data. The measurement uses a
likelihood-based method in a sample highly enriched in tt¯
events. The topology of the t→ Wb decays is exploited to
simultaneously measure both the jet flavour composition of
the sample and the efficiency in a transverse momentum range
from 20 to 600 GeV. The efficiency measurement is
subsequently compared with that predicted by the simulation.
The data used in this measurement, corresponding to a total
integrated luminosity of 80.5 fb - 1, were collected in
proton–proton collisions during the years 2015–2017 at a
centre-of-mass energy s= 13 TeV. By simultaneously
extracting both the efficiency and jet flavour composition,
this measurement significantly improves the precision
compared to previous results, with uncertainties ranging
from 1 to 8% depending on the jet transverse
momentum.},
Doi = {10.1140/epjc/s10052-019-7450-8},
Key = {fds356564}
}
@article{fds310336,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amaral
Coutinho, Y and Amelung, C and Amor Dos Santos and SP and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B},
Title = {ATLAS Collaboration},
Journal = {Nuclear Physics A},
Volume = {932},
Pages = {572-594},
Publisher = {Elsevier BV},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1016/S0375-9474(14)00601-0},
Doi = {10.1016/S0375-9474(14)00601-0},
Key = {fds310336}
}
@article{fds350339,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
Title = {ATLAS data quality operations and performance for 2015-2018
data-taking},
Journal = {Journal of Instrumentation},
Volume = {15},
Number = {4},
Year = {2020},
Month = {April},
url = {http://dx.doi.org/10.1088/1748-0221/15/04/P04003},
Abstract = {The ATLAS detector at the Large Hadron Collider reads out
particle collision data from over 100 million electronic
channels at a rate of approximately 100 kHz, with a
recording rate for physics events of approximately 1 kHz.
Before being certified for physics analysis at computer
centres worldwide, the data must be scrutinised to ensure
they are clean from any hardware or software related issues
that may compromise their integrity. Prompt identification
of these issues permits fast action to investigate, correct
and potentially prevent future such problems that could
render the data unusable. This is achieved through the
monitoring of detector-level quantities and reconstructed
collision event characteristics at key stages of the data
processing chain. This paper presents the monitoring and
assessment procedures in place at ATLAS during 2015-2018
data-taking. Through the continuous improvement of
operational procedures, ATLAS achieved a high data quality
efficiency, with 95.6% of the recorded proton-proton
collision data collected at s=13 TeV certified for physics
analysis.},
Doi = {10.1088/1748-0221/15/04/P04003},
Key = {fds350339}
}
@article{fds372327,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev,
V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {ATLAS flavour-tagging algorithms for the LHC Run 2 pp
collision dataset},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11699-1},
Abstract = {The flavour-tagging algorithms developed by the ATLAS
Collaboration and used to analyse its dataset of s=13 TeV pp
collisions from Run 2 of the Large Hadron Collider are
presented. These new tagging algorithms are based on
recurrent and deep neural networks, and their performance is
evaluated in simulated collision events. These developments
yield considerable improvements over previous jet-flavour
identification strategies. At the 77% b-jet identification
efficiency operating point, light-jet (charm-jet) rejection
factors of 170 (5) are achieved in a sample of simulated
Standard Model tt¯ events; similarly, at a c-jet
identification efficiency of 30%, a light-jet (b-jet)
rejection factor of 70 (9) is obtained.},
Doi = {10.1140/epjc/s10052-023-11699-1},
Key = {fds372327}
}
@article{fds307798,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G},
Title = {ATLAS measurements of the properties of jets for boosted
particle searches},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.86.072006},
Abstract = {Measurements are presented of the properties of high
transverse momentum jets, produced in proton-proton
collisions at a center-of-mass energy of √s=7TeV. The data
correspond to an integrated luminosity of 35pb -1 and were
collected with the ATLAS detector in 2010. Jet mass, width,
eccentricity, planar flow and angularity are measured for
jets reconstructed using the anti-kt algorithm with distance
parameters R=0.6 and 1.0, with transverse momentum pT>300GeV
and pseudorapidity |η|<2. The measurements are compared to
the expectations of Monte Carlo generators that match
leading-logarithmic parton showers to leading-order, or
next-to-leading-order, matrix elements. The generators
describe the general features of the jets, although
discrepancies are observed in some distributions. © 2012
CERN, for the ATLAS Collaboration Published by the American
Physical Society under the terms of the http://creativecommons.
org/licenses/by/3.0/ Creative Commons Attribution 3.0
License. Further distribution of this work must maintain
attribution to the author(s) and the published article's
title, journal citation, and DOI.},
Doi = {10.1103/PhysRevD.86.072006},
Key = {fds307798}
}
@article{fds346168,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black,
CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
Title = {ATLAS Run 1 searches for direct pair production of
third-generation squarks at the Large Hadron
Collider.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {10},
Pages = {510},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3726-9},
Abstract = {This paper reviews and extends searches for the direct pair
production of the scalar supersymmetric partners of the top
and bottom quarks in proton-proton collisions collected by
the ATLAS collaboration during the LHC Run 1. Most of the
analyses use 20 [Formula: see text] of collisions at a
centre-of-mass energy of [Formula: see text] TeV, although
in some case an additional [Formula: see text] of collision
data at [Formula: see text] TeV are used. New analyses are
introduced to improve the sensitivity to specific regions of
the model parameter space. Since no evidence of
third-generation squarks is found, exclusion limits are
derived by combining several analyses and are presented in
both a simplified model framework, assuming simple decay
chains, as well as within the context of more elaborate
phenomenological supersymmetric models.},
Doi = {10.1140/epjc/s10052-015-3726-9},
Key = {fds346168}
}
@article{fds307661,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {ATLAS search for a heavy gauge boson decaying to a charged
lepton and a neutrino in pp collisions at √s =7
TeV},
Journal = {European Physical Journal C},
Volume = {72},
Number = {12},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2241-5},
Abstract = {The ATLAS detector at the LHC is used to search for
high-mass states, such as heavy charged gauge bosons (Wʹ),
decaying to a charged lepton (electron or muon) and a
neutrino. Results are presented based on the analysis of pp
collisions at a center-of-mass energy of 7 TeV corresponding
to an integrated luminosity of 4.7 fb−1. No excess beyond
Standard Model expectations is observed. AWʹ with
Sequential Standard Model couplings is excluded at the 95%
credibility level for masses up to 2.55 TeV. Excited chiral
bosons (W*) with equivalent coupling strength are excluded
for masses up to 2.42 TeV.},
Doi = {10.1140/epjc/s10052-012-2241-5},
Key = {fds307661}
}
@article{fds317300,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {ATLAS search for new phenomena in dijet mass and angular
distributions using pp collisions at √s = 7
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {1},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2013)029},
Abstract = {Mass and angular distributions of dijets produced in LHC
proton-proton collisions at a centre-of-mass energy √s =
7TeV have been studied with the ATLAS detector using the
full 2011 data set with an integrated luminosity of 4.8
fb-1. Dijet masses up to ~ 4.0TeV have been probed. No
resonance-like features have been observed in the dijet mass
spectrum, and all angular distributions are consistent with
the predictions of QCD. Exclusion limits on six hypotheses
of new phenomena have been set at 95% CL in terms of mass or
energy scale, as appropriate. These hypotheses include
excited quarks below 2.83 TeV, colour octet scalars below
1.86TeV, heavy W bosons below 1.68 TeV, string resonances
below 3.61 TeV, quantum black holes with six extra
space-time dimensions for quantum gravity scales below 4.11
TeV, and quark contact interactions below a compositeness
scale of 7.6 TeV in a destructive interference
scenario.},
Doi = {10.1007/JHEP01(2013)029},
Key = {fds317300}
}
@article{fds362443,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari,
N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
Title = {AtlFast3: The Next Generation of Fast Simulation in
ATLAS},
Journal = {Computing and Software for Big Science},
Volume = {6},
Number = {1},
Year = {2022},
Month = {December},
url = {http://dx.doi.org/10.1007/s41781-021-00079-7},
Abstract = {The ATLAS experiment at the Large Hadron Collider has a
broad physics programme ranging from precision measurements
to direct searches for new particles and new interactions,
requiring ever larger and ever more accurate datasets of
simulated Monte Carlo events. Detector simulation with
Geant4 is accurate but requires significant CPU resources.
Over the past decade, ATLAS has developed and utilized tools
that replace the most CPU-intensive component of the
simulation—the calorimeter shower simulation—with faster
simulation methods. Here, AtlFast3, the next generation of
high-accuracy fast simulation in ATLAS, is introduced.
AtlFast3 combines parameterized approaches with
machine-learning techniques and is deployed to meet current
and future computing challenges, and simulation needs of the
ATLAS experiment. With highly accurate performance and
significantly improved modelling of substructure within
jets, AtlFast3 can simulate large numbers of events for a
wide range of physics processes.},
Doi = {10.1007/s41781-021-00079-7},
Key = {fds362443}
}
@article{fds374561,
Author = {ATLAS Collaboration},
Title = {Author Correction: A detailed map of Higgs boson
interactions by the ATLAS experiment ten years after the
discovery.},
Journal = {Nature},
Volume = {623},
Number = {7985},
Pages = {E5},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1038/s41586-023-06248-5},
Doi = {10.1038/s41586-023-06248-5},
Key = {fds374561}
}
@article{fds346179,
Author = {Gupta, SK and Kotwal, J and Kotwal, A and Dhall, A and Garg,
S},
Title = {Authors' response.},
Journal = {The Indian journal of medical research},
Volume = {138},
Number = {4},
Pages = {562-563},
Year = {2013},
Month = {October},
Key = {fds346179}
}
@article{fds323670,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arduini, G and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Beam-induced and cosmic-ray backgrounds observed in the
ATLAS detector during the LHC 2012 proton-proton running
period},
Journal = {Journal of Instrumentation},
Volume = {11},
Number = {5},
Pages = {P05013-P05013},
Publisher = {IOP Publishing},
Year = {2016},
Month = {May},
url = {http://dx.doi.org/10.1088/1748-0221/11/05/P05013},
Abstract = {This paper discusses various observations on beam-induced
and cosmic-ray backgrounds in the ATLAS detector during the
LHC 2012 proton-proton run. Building on published results
based on 2011 data, the correlations between background and
residual pressure of the beam vacuum are revisited. Ghost
charge evolution over 2012 and its role for backgrounds are
evaluated. New methods to monitor ghost charge with beam-gas
rates are presented and observations of LHC abort gap
population by ghost charge are discussed in detail. Fake
jets from colliding bunches and from ghost charge are
analysed with improved methods, showing that ghost charge in
individual radio-frequency buckets of the LHC can be
resolved. Some results of two short periods of dedicated
cosmic-ray background data-taking are shown; in particular
cosmic-ray muon induced fake jet rates are compared to Monte
Carlo simulations and to the fake jet rates from beam
background. A thorough analysis of a particular LHC fill,
where abnormally high background was observed, is presented.
Correlations between backgrounds and beam intensity losses
in special fills with very high β∗ are
studied.},
Doi = {10.1088/1748-0221/11/05/P05013},
Key = {fds323670}
}
@article{fds308168,
Author = {Hossenfelder, S and Bleicher, M and Hofmann, S and Stöcker, H and Kotwal, AV},
Title = {Black hole relics in large extra dimensions},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {566},
Number = {3-4},
Pages = {233-239},
Publisher = {Elsevier BV},
Year = {2003},
Month = {July},
url = {http://dx.doi.org/10.1016/S0370-2693(03)00835-9},
Abstract = {Recent calculations applying statistical mechanics indicate
that in a setting with compactified large extra dimensions a
black hole might evolve into a (quasi-)stable state with
mass close to the new fundamental scale Mf. Black holes and
therefore their relics might be produced at the LHC in the
case of extra-dimensional topologies. In this energy regime,
Hawking's evaporation scenario is modified due to energy
conservation and quantum effects. We reanalyse the
evaporation of small black holes including the quantisation
of the emitted radiation due to the finite surface of the
black hole. It is found that observable stable black hole
relics with masses ∼ 1-3Mf would form which could be
identified by a delayed single jet with a corresponding hard
momentum kick to the relic and by ionisation, e.g., in a
TPC. © 2003 Published by Elsevier B.V.},
Doi = {10.1016/S0370-2693(03)00835-9},
Key = {fds308168}
}
@article{fds346176,
Author = {Singh, R and Prakash, M and Dubey, R and Roy, K and Kotwal, A and Mahen,
A},
Title = {Body composition parameters as correlates of coronary artery
disease.},
Journal = {The Indian journal of medical research},
Volume = {138},
Number = {6},
Pages = {1016-1019},
Year = {2013},
Month = {December},
Abstract = {<h4>Background & objectives</h4>Obesity is a major risk
factor for cardiovascular disease (CAD). This study was
aimed to assess the risk for CAD determined by certain new
and conventional body composition parameters such as
visceral fat area (VFA), body mass index (BMI), waist to hip
ratio (WHR), etc.<h4>Methods</h4>We did an age and sex
matched case-control study of acute myocardial infarction
with 100 participants in a tertiary care hospital (50 cases
and 50 controls) representing the serving army personnel.
The relation between VFA, per cent body fat (PBF), BMI,
waist and hip circumferences, and WHR to CAD was
assessed.<h4>Results</h4>The study showed that there was a
significantly increased risk for CAD associated with VFA
(OR: 5.67; 95% CI: 1.96, 16.95), WHR (7.07; 2.19, 24.27),
waist circumference (WC) (2.63; 1.05, 6.66) and BMI (2.53;
1.03, 6.26).<h4>Interpretation & conclusions</h4>In
conclusion, increased VFA, BMI, WHR and WC showed an
association with CAD. VFA is a good index for assessing not
only visceral fat accumulation but also cardiovascular risk
factors.},
Key = {fds346176}
}
@article{fds374028,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
Title = {Calibration of the light-flavour jet mistagging efficiency
of the b-tagging algorithms with Z+jets events using 139 fb
- 1 of ATLAS proton–proton collision data at
√s=13 TeV},
Journal = {European Physical Journal C},
Volume = {83},
Number = {8},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11736-z},
Abstract = {The identification of b-jets, referred to as b-tagging, is
an important part of many physics analyses in the ATLAS
experiment at the Large Hadron Collider and an accurate
calibration of its performance is essential for high-quality
physics results. This publication describes the calibration
of the light-flavour jet mistagging efficiency in a data
sample of proton–proton collision events at s=13 TeV
corresponding to an integrated luminosity of 139 fb - 1 .
The calibration is performed in a sample of Z bosons
produced in association with jets. Due to the low mistagging
efficiency for light-flavour jets, a method which uses
modified versions of the b-tagging algorithms referred to as
flip taggers is used in this work. A fit to the
jet-flavour-sensitive secondary-vertex mass is performed to
extract a scale factor from data, to correct the
light-flavour jet mistagging efficiency in Monte Carlo
simulations, while simultaneously correcting the b-jet
efficiency. With this procedure, uncertainties coming from
the modeling of jets from heavy-flavour hadrons are
considerably lower than in previous calibrations of the
mistagging scale factors, where they were dominant. The
scale factors obtained in this calibration are consistent
with unity within uncertainties.},
Doi = {10.1140/epjc/s10052-023-11736-z},
Key = {fds374028}
}
@article{fds308166,
Author = {Affolder, T and Allspach, D and Ambrose, D and Bialek, J and Bokhari, W and Brozovic, M and Binkley, M and Burkett, K and Byon Wagner and A and Cogswell, F and Dressnandt, N and Feng, Z and Franklin, M and Galtieri,
L and Gerdes, DW and Greenwood, J and Guarino, V and Guimaraes, J and da
Costa, R and Haggerty, C},
Title = {CDF Central Outer Tracker},
Journal = {Nuclear Instruments and Methods in Physics Research Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {526},
Number = {3},
Pages = {249-299},
Publisher = {Elsevier BV},
Year = {2004},
Month = {July},
url = {http://dx.doi.org/10.1016/j.nima.2004.02.020},
Abstract = {The Central Outer Tracker is a large cylindrical drift
chamber constructed to replace Collider Detector at
Fermilab's original central drift chamber for the higher
luminosity expected for Run 2 at the Fermilab Tevatron. The
chamber's drift properties are described in the context of
meeting the operating requirements for Run 2. The design and
construction of the chamber, the front- end readout
electronics, and the high-voltage system are described in
detail. Wire aging considerations are also
discussed.},
Doi = {10.1016/j.nima.2004.02.020},
Key = {fds308166}
}
@article{fds310117,
Author = {Baranovski, A and Benjamin, D and Cooper, G and Farrington, S and Genser, K and Hou, S and Hsieh, T and Kotwal, A and Lipeles, E and Murat,
P and Norman, M and Robson, A and Sfiligoi, I and Snider, R and Stelzer, B and Syu, J and Timm, S and Vataga, E and Wolbers, S and Zhang,
D},
Title = {CDF II Production Farm Project},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {572},
Number = {1 SPEC. ISS.},
Pages = {399-401},
Publisher = {Elsevier BV},
Year = {2007},
Month = {March},
url = {http://dx.doi.org/10.1016/j.nima.2006.11.048},
Abstract = {We describe the architecture and discuss our operational
experience in running the off-line reconstruction farm of
the CDFII experiment. The Linux PC-based farm performs a
wide set of tasks, ranging from producing calibrations and
primary event reconstruction to large scale ntuple
production. The farm control software uses a standard Condor
toolkit [The Condor project page, 〈http://www.cs.wisc.edu/condor〉]
and the data handling part is based on SAM (Sequential
Access via Metadata [Sequential data Access via Meta-data
〈http://d0db.fnal.gov/sam/〉]) software. During its
lifetime, the CDFII experiment will integrate a large amount
of data (several petabytes) and the data processing chain is
one of the key components of the successful physics program
of the experiment. © 2006 Elsevier B.V. All rights
reserved.},
Doi = {10.1016/j.nima.2006.11.048},
Key = {fds310117}
}
@article{fds310260,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Centrality and rapidity dependence of inclusive jet
production in √sNN =5 .02 TeV proton–lead collisions
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {748},
Pages = {392-413},
Publisher = {Elsevier BV},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2015.07.023},
Abstract = {Measurements of the centrality and rapidity dependence of
inclusive jet production in sNN=5.02 TeV proton–lead
(p+Pb) collisions and the jet cross-section in s=2.76 TeV
proton–proton collisions are presented. These quantities
are measured in datasets corresponding to an integrated
luminosity of 27.8 nb−1 and 4.0 pb−1, respectively,
recorded with the ATLAS detector at the Large Hadron
Collider in 2013. The p+Pb collision centrality was
characterised using the total transverse energy measured in
the pseudorapidity interval −4.9 <η <−3.2 in the
direction of the lead beam. Results are presented for the
double-differential per-collision yields as a function of
jet rapidity and transverse momentum (pT) for minimum-bias
and centrality-selected p+Pb collisions, and are compared to
the jet rate from the geometric expectation. The total jet
yield in minimum-bias events is slightly enhanced above the
expectation in a pT-dependent manner but is consistent with
the expectation within uncertainties. The ratios of jet
spectra from different centrality selections show a strong
modification of jet production at all pT at forward
rapidities and for large pT at mid-rapidity, which manifests
as a suppression of the jet yield in central events and an
enhancement in peripheral events. These effects imply that
the factorisation between hard and soft processes is
violated at an unexpected level in proton–nucleus
collisions. Furthermore, the modifications at forward
rapidities are found to be a function of the total jet
energy only, implying that the violations may have a simple
dependence on the hard parton–parton kinematics.},
Doi = {10.1016/j.physletb.2015.07.023},
Key = {fds310260}
}
@article{fds315923,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Centrality, rapidity, and transverse momentum dependence of
isolated prompt photon production in lead-lead collisions at
sNN =2.76 TeV measured with the ATLAS detector},
Journal = {Physical Review C},
Volume = {93},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {March},
ISSN = {2469-9985},
url = {http://dx.doi.org/10.1103/PhysRevC.93.034914},
Abstract = {Prompt photon production in sNN=2.76-TeV Pb+Pb collisions
has been measured by the ATLAS experiment at the Large
Hadron Collider using data collected in 2011 with an
integrated luminosity of 0.14 nb-1. Inclusive photon yields,
scaled by the mean nuclear thickness function, are presented
as a function of collision centrality and transverse
momentum in two pseudorapidity intervals, |η|<1.37 and
1.52≤|η|<2.37. The scaled yields in the two
pseudorapidity intervals, as well as the ratios of the
forward yields to those at midrapidity, are compared to the
expectations from next-to-leading-order perturbative QCD
(pQCD) calculations. The measured cross sections agree well
with the predictions for proton-proton collisions within
statistical and systematic uncertainties. Both the yields
and the ratios are also compared to two other pQCD
calculations, one which uses the isospin content appropriate
to colliding lead nuclei and another which includes nuclear
modifications to the nucleon parton distribution
functions.},
Doi = {10.1103/PhysRevC.93.034914},
Key = {fds315923}
}
@article{fds316848,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
S},
Title = {Characterisation and mitigation of beam-induced backgrounds
observed in the ATLAS detector during the 2011 proton-proton
run},
Journal = {Journal of Instrumentation},
Volume = {8},
Number = {7},
Pages = {P07004-P07004},
Publisher = {IOP Publishing},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/8/07/P07004},
Abstract = {This paper presents a summary of beam-induced backgrounds
observed in the ATLAS detector and discusses methods to tag
and remove background contaminated events in data.
Triggerrate based monitoring of beam-related backgrounds is
presented. The correlations of backgrounds with machine
conditions, such as residual pressure in the beam-pipe, are
discussed. Results from dedicated beam-background
simulations are shown, and their qualitative agreement with
data is evaluated. Data taken during the passage of
unpaired, i.e. non-colliding, proton bunches is used to
obtain background-enriched data samples. These are used to
identify characteristic features of beam-induced
backgrounds, which then are exploited to develop dedicated
background tagging tools. These tools, based on observables
in the Pixel detector, the muon spectrometer and the
calorimeters, are described in detail and their efficiencies
are evaluated. Finally an example of an application of these
techniques to a monojet analysis is given, which
demonstrates the importance of such event cleaning
techniques for some new physics searches.},
Doi = {10.1088/1748-0221/8/07/P07004},
Key = {fds316848}
}
@article{fds321096,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel,
C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund,
OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan,
AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel,
O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio,
D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez,
SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El
Moursli, RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A},
Title = {Charged-particle distributions at low transverse momentum in
[Formula: see text] TeV pp interactions measured
with the ATLAS detector at the LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {9},
Pages = {502},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4335-y},
Abstract = {Measurements of distributions of charged particles produced
in proton-proton collisions with a centre-of-mass energy of
13 TeV are presented. The data were recorded by the ATLAS
detector at the LHC and correspond to an integrated
luminosity of 151 [Formula: see text]. The particles are
required to have a transverse momentum greater than 100 MeV
and an absolute pseudorapidity less than 2.5. The
charged-particle multiplicity, its dependence on transverse
momentum and pseudorapidity and the dependence of the mean
transverse momentum on multiplicity are measured in events
containing at least two charged particles satisfying the
above kinematic criteria. The results are corrected for
detector effects and compared to the predictions from
several Monte Carlo event generators.},
Doi = {10.1140/epjc/s10052-016-4335-y},
Key = {fds321096}
}
@article{fds321118,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi,
S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
Title = {Charged-particle distributions in pp interactions at
[Formula: see text] measured with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {7},
Pages = {403},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4203-9},
Abstract = {This paper presents measurements of distributions of charged
particles which are produced in proton-proton collisions at
a centre-of-mass energy of [Formula: see text] and recorded
by the ATLAS detector at the LHC. A special dataset recorded
in 2012 with a small number of interactions per beam
crossing (below 0.004) and corresponding to an integrated
luminosity of 160 [Formula: see text] was used. A
minimum-bias trigger was utilised to select a data sample of
more than 9 million collision events. The multiplicity,
pseudorapidity, and transverse momentum distributions of
charged particles are shown in different regions of
kinematics and charged-particle multiplicity, including
measurements of final states at high multiplicity. The
results are corrected for detector effects and are compared
to the predictions of various Monte Carlo event generator
models which simulate the full hadronic final
state.},
Doi = {10.1140/epjc/s10052-016-4203-9},
Key = {fds321118}
}
@article{fds315919,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Charged-particle distributions in √s=13 TeV pp
interactions measured with the ATLAS detector at the
LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {758},
Pages = {67-88},
Publisher = {Elsevier BV},
Year = {2016},
Month = {July},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2016.04.050},
Abstract = {Charged-particle distributions are measured in
proton–proton collisions at a centre-of-mass energy of 13
TeV, using a data sample of nearly 9 million events,
corresponding to an integrated luminosity of 170 μb−1,
recorded by the ATLAS detector during a special Large Hadron
Collider fill. The charged-particle multiplicity, its
dependence on transverse momentum and pseudorapidity and the
dependence of the mean transverse momentum on the
charged-particle multiplicity are presented. The
measurements are performed with charged particles with
transverse momentum greater than 500 MeV and absolute
pseudorapidity less than 2.5, in events with at least one
charged particle satisfying these kinematic requirements.
Additional measurements in a reduced phase space with
absolute pseudorapidity less than 0.8 are also presented, in
order to compare with other experiments. The results are
corrected for detector effects, presented as particle-level
distributions and are compared to the predictions of various
Monte Carlo event generators.},
Doi = {10.1016/j.physletb.2016.04.050},
Key = {fds315919}
}
@booklet{Abbott97,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and di Loreto, G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Color coherent radiation in multijet events from
pp- collisions at √s = 1.8 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {414},
Number = {3-4},
Pages = {419-427},
Publisher = {Elsevier BV},
Year = {1997},
Month = {November},
url = {http://dx.doi.org/10.1016/S0370-2693(97)01190-8},
Abstract = {We report on a study of color coherence effects in pp-
collisions at a center of mass energy √s = 1.8 TeV. The
data were collected with the DØ detector during the
1992-1993 run of the Fermilab Tevatron Collider. We observe
the presence of initial-to-final state color interference
with the spatial correlations between soft and hard jets in
multijet events in the central and in forward pseudorapidity
regions. The results are compared to Monte Carlo simulations
with different color coherence implementations and to the
predictions of script O sign(α3s) QCD calculations. © 1997
Elsevier Science B.V.},
Doi = {10.1016/S0370-2693(97)01190-8},
Key = {Abbott97}
}
@article{fds307799,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Asman, B and Atkins, S and Atramentov, O and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barreto, J and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Belanger-Champagne, C and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bezzubov, VA and Bhatia, S and Bhatnagar, V and Bhatti, A and Bhat, PC and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Brooijmans, G and Bross, A and Brown, D and Brown, J and Brucken, E and Bu,
XB},
Title = {Combination of CDF and D0 measurements of the W boson
helicity in top quark decays},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.85.071106},
Abstract = {We report the combination of recent measurements of the
helicity of the W boson from top quark decay by the CDF and
D0 collaborations, based on data samples corresponding to
integrated luminosities of 2.7-5.4fb -1 of pp̄ collisions
collected during Run II of the Fermilab Tevatron collider.
Combining measurements that simultaneously determine the
fractions of W bosons with longitudinal (f 0) and
right-handed (f +) helicities, we find f
0=0.722±0.081[±0.062(stat)±0.052(syst)] and f
+=-0.033±0.046[±0.034(stat)±0.031(syst)]. Combining
measurements where one of the helicity fractions is fixed to
the value expected in the standard model, we find f
0=0.682±0. 057[±0.035(stat)±0.046(syst)] for fixed f +
and f +=-0.015±0.035[±0.018(stat)±0.030(syst)] for fixed
f 0. The results are consistent with standard model
expectations. © 2012 American Physical Society.},
Doi = {10.1103/PhysRevD.85.071106},
Key = {fds307799}
}
@article{fds308163,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Acosta, D and Adams, DL and Adams, M and Affolder, T and Ahmed, SN and Akimoto, H and Akopian, A and Albrow, MG and Alexeev, GD and Alton, A and Alves, GA and Amaral, P and Ambrose, D and Amendolia, SR and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arnoud, Y and Arisawa, T and Artikov, A and Asakawa, T and Avila, C and Ashmanskas, W and Atac, M and Azfar, F and Azzi-Bacchetta, P and Babintsev, VV and Babukhadia, L and Bacchetta, N and Bachacou, H and Bacon, TC and Baden,
A and Badgett, W and Baffioni, S and Bailey, MW and Bailey, S and Baldin,
B and Balm, PW and Banerjee, S and Barbaro, P and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Baroiant,
S and Barone, M and Barreto, J and Bartlett, JF and Bassler, U and Bauer,
D and Bauer, G and Bean, A and Beaudette, F and Bedeschi, F and Behari, S and Begel, M and Belforte, S and Bell, WH and Bellettini, G and Bellinger,
J and Belyaev, A and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Beri, SB and Bernardi, G and Bertram, I and Berryhill, J and Besson, A and Beuselinck, R and Bevensee, B and Bezzubov, VA and Bhat,
PC and Bhatnagar, V and Bhattacharjee, M and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blazey, G and Blekman, F and Blessing, S and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Boehnlein, A and Bojko,
NI},
Title = {Combination of CDF and D0 results on the [Formula Presented]
boson mass and width},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {70},
Number = {9},
Pages = {17},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {Fall},
url = {http://dx.doi.org/10.1103/PhysRevD.70.092008},
Abstract = {The results based on 1992–95 data (Run 1) from the CDF and
D0 experiments on the measurements of the [Formula
Presented] boson mass and width are presented, along with
the combined results. We report a Tevatron collider average
[Formula Presented]. We also report the Tevatron collider
average of the directly measured [Formula Presented] boson
width [Formula Presented]. We describe a new joint analysis
of the direct [Formula Presented] mass and width
measurements. Assuming the validity of the standard model,
we combine the directly measured [Formula Presented] boson
width with the width extracted from the ratio of [Formula
Presented] and [Formula Presented] boson leptonic partial
cross sections. This combined result for the Tevatron is
[Formula Presented]. Finally, we use the measurements of the
direct total [Formula Presented] width and the leptonic
branching ratio to extract the leptonic partial width
[Formula Presented]. © 2004 The American Physical
Society.},
Doi = {10.1103/PhysRevD.70.092008},
Key = {fds308163}
}
@article{fds307577,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Beecher, D and Begalli, M and Behari, S and Bellantoni,
L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon,
M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti,
A and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Boudreau, J and Boveia,
A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg,
C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd,
HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P},
Title = {Combination of CDF and D0 W-Boson mass measurements},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {5},
Pages = {052018},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.88.052018},
Abstract = {We summarize and combine direct measurements of the mass of
the W boson in √s=1.96 TeV proton-antiproton collision
data collected by CDF and D0 experiments at the Fermilab
Tevatron Collider. Earlier measurements from CDF and D0 are
combined with the two latest, more precise measurements: a
CDF measurement in the electron and muon channels using data
corresponding to 2.2 fb-1 of integrated luminosity, and a D0
measurement in the electron channel using data corresponding
to 4.3 fb-1 of integrated luminosity. The resulting Tevatron
average for the mass of the W boson is M W=80387±16 MeV.
Including measurements obtained in electron-positron
collisions at LEP yields the most precise value of M
W=80385±15 MeV. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.052018},
Key = {fds307577}
}
@article{fds356706,
Author = {Sirunyan, AM and Tumasyan, A and Adam, W and Ambrogi, F and Asilar, E and Bergauer, T and Brandstetter, J and Brondolin, E and Dragicevic, M and Erö, J and Escalante Del Valle and A and Flechl, M and Friedl, M and Frühwirth, R and Ghete, VM and Grossmann, J and Hrubec, J and Jeitler,
M and König, A and Krammer, N and Krätschmer, I and Liko, D and Madlener,
T and Mikulec, I and Pree, E and Rad, N and Rohringer, H and Schieck, J and Schöfbeck, R and Spanring, M and Spitzbart, D and Taurok, A and Waltenberger, W and Wittmann, J and Wulz, CE and Zarucki, M and Chekhovsky, V and Mossolov, V and Suarez Gonzalez and J and De Wolf and EA and Di Croce and D and Janssen, X and Lauwers, J and Van De Klundert and M and Van
Haevermaet, H and Van Mechelen and P and Van Remortel and N and Abu Zeid,
S and Blekman, F and D’hondt, J and De Bruyn and I and De Clercq and J and Deroover, K and Flouris, G and Lontkovskyi, D and Lowette, S and Marchesini, I and Moortgat, S and Moreels, L and Python, Q and Skovpen,
K and Tavernier, S and Van Doninck and W and Van Mulders and P and Van Parijs,
I and Beghin, D and Bilin, B and Brun, H and Clerbaux, B and De Lentdecker,
G and Delannoy, H and Dorney, B and Fasanella, G and Favart, L and Goldouzian, R and Grebenyuk, A and Kalsi, AK and Lenzi, T and Luetic, J and Maerschalk, T and Marinov, A and Seva, T and Starling, E and Vander
Velde, C and Vanlaer, P and Vannerom, D and Yonamine, R and Zenoni, F and Cornelis, T and Dobur, D and Fagot, A and Gul, M and Khvastunov, I and Poyraz, D and Roskas, C and Salva, S and Tytgat, M and Verbeke, W and Zaganidis, N and Bakhshiansohi, H},
Title = {Combination of inclusive and differential tt¯ charge
asymmetry measurements using ATLAS and CMS data at √s = 7
and 8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {4},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP04(2018)033},
Abstract = {This paper presents combinations of inclusive and
differential measurements of the charge asymmetry (AC) in
top quark pair (tt) events with a lepton+jets signature by
the ATLAS and CMS Collaborations, using data from LHC
proton-proton collisions at centreof- mass energies of 7 and
8TeV. The data correspond to integrated luminosities of
about 5 and 20 fb–1for each experiment, respectively. The
resulting combined LHC measurements of the inclusive charge
asymmetry are ACLHC7= 0:005±0:007 (stat) ±0:006 (syst) at
7TeV and ACLHC7= 0:0055 ± 0:0023 (stat) ± 0:0025 (syst) at
8TeV. These values, as well as the combination of AC
measurements as a function of the invariant mass of the
[formula presented] system at 8TeV, are consistent with the
respective standard model predictions.},
Doi = {10.1007/JHEP04(2018)033},
Key = {fds356706}
}
@article{fds307542,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu,
A},
Title = {Combination of measurements of the top-quark pair production
cross section from the Tevatron Collider},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072001},
Abstract = {We combine six measurements of the inclusive top-quark pair
(tt̄) production cross section (σtt̄) from data collected
with the CDF and D0 detectors at the Fermilab Tevatron with
proton-antiproton collisions at s=1.96TeV. The data
correspond to integrated luminosities of up to 8.8fb-1. We
obtain a value of σtt̄=7.60±0.41pb for a top-quark mass
of mt=172.5GeV. The contributions to the uncertainty are
0.20 pb from statistical sources, 0.29 pb from systematic
sources, and 0.21 pb from the uncertainty on the integrated
luminosity. The result is in good agreement with the
standard model expectation of 7.35-0.33+0.28pb at
next-to-next-to-leading order and next-to-next-to leading
logarithms in perturbative QCD. © 2014 American Physical
Society.},
Doi = {10.1103/PhysRevD.89.072001},
Key = {fds307542}
}
@article{fds356659,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Combination of searches for heavy resonances decaying into
bosonic and leptonic final states using 36 fb-1 of
proton-proton collision data at s =13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {98},
Number = {5},
Year = {2018},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.98.052008},
Abstract = {Searches for new heavy resonances decaying into different
pairings of W, Z, or Higgs bosons, as well as directly into
leptons, are presented using a data sample corresponding to
36.1 fb-1 of pp collisions at s=13 TeV collected during 2015
and 2016 with the ATLAS detector at the CERN Large Hadron
Collider. Analyses selecting bosonic decay modes in the
qqqq, ννqq, ℓνqq, ℓℓqq, ℓνℓν, ℓℓνν,
ℓνℓℓ, ℓℓℓℓ, qqbb, ννbb, ℓνbb, and
ℓℓbb final states are combined, searching for a
narrow-width resonance. Likewise, analyses selecting the
leptonic ℓν and ℓℓ final states are also combined.
These two sets of analyses are then further combined. No
significant deviation from the Standard Model predictions is
observed. Three benchmark models are tested: a model
predicting the existence of a new heavy scalar singlet, a
simplified model predicting a heavy vector-boson triplet,
and a bulk Randall-Sundrum model with a heavy spin-2
Kaluza-Klein excitation of the graviton. Cross section
limits are set at the 95% confidence level using an
asymptotic approximation and are compared with predictions
for the benchmark models. These limits are also expressed in
terms of constraints on couplings of the heavy vector-boson
triplet to quarks, leptons, and the Higgs boson. The data
exclude a heavy vector-boson triplet with mass below 5.5 TeV
in a weakly coupled scenario and 4.5 TeV in a strongly
coupled scenario, as well as a Kaluza-Klein graviton with
mass below 2.3 TeV.},
Doi = {10.1103/PhysRevD.98.052008},
Key = {fds356659}
}
@article{fds356546,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R},
Title = {Combination of searches for Higgs boson pairs in pp
collisions at s=13TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {800},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2019.135103},
Abstract = {This letter presents a combination of searches for Higgs
boson pair production using up to 36.1 fb−1 of
proton–proton collision data at a centre-of-mass energy
s=13 TeV recorded with the ATLAS detector at the LHC. The
combination is performed using six analyses searching for
Higgs boson pairs decaying into the bb¯bb¯, bb¯W+W−,
bb¯τ+τ−, W+W−W+W−, bb¯γγ and W+W−γγ final
states. Results are presented for non-resonant and resonant
Higgs boson pair production modes. No statistically
significant excess in data above the Standard Model
predictions is found. The combined observed (expected) limit
at 95% confidence level on the non-resonant Higgs boson pair
production cross-section is 6.9 (10) times the predicted
Standard Model cross-section. Limits are also set on the
ratio (κλ) of the Higgs boson self-coupling to its
Standard Model value. This ratio is constrained at 95%
confidence level in observation (expectation) to
−5.0<κλ<12.0 (−5.8<κλ<12.0). In addition, limits are
set on the production of narrow scalar resonances and spin-2
Kaluza–Klein Randall–Sundrum gravitons. Exclusion
regions are also provided in the parameter space of the
habemus Minimal Supersymmetric Standard Model and the
Electroweak Singlet Model.},
Doi = {10.1016/j.physletb.2019.135103},
Key = {fds356546}
}
@article{fds372126,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH},
Title = {Combination of searches for invisible decays of the Higgs
boson using 139 fb−1 of proton-proton collision
data at s=13 TeV collected with the ATLAS
experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {842},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137963},
Abstract = {Many extensions of the Standard Model predict the production
of dark matter particles at the LHC. Sufficiently light dark
matter particles may be produced in decays of the Higgs
boson that would appear invisible to the detector. This
Letter presents a statistical combination of searches for
H→invisible decays where multiple production modes of the
Standard Model Higgs boson are considered. These searches
are performed with the ATLAS detector using 139 fb−1 of
proton–proton collisions at a centre–of–mass energy of
[Formula presented] at the LHC. In combination with the
results at [Formula presented] and [Formula presented], an
upper limit on the H→invisible branching ratio of 0.107
(0.077) at the 95% confidence level is observed (expected).
These results are also interpreted in the context of models
where the 125 GeV Higgs boson acts as a portal to dark
matter, and limits are set on the scattering cross-section
of weakly interacting massive particles and
nucleons.},
Doi = {10.1016/j.physletb.2023.137963},
Key = {fds372126}
}
@article{fds347443,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster,
AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey,
AJ and Bailey, VR and Baines, JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek,
P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay,
A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Batool,
B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Besson,
N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi,
R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bitadze, A and Bittrich, C and Bjergaard, DM and Black,
JE and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burr, JTP and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carter, JWS and Casado, MP and Casha, AF and Casper, DW and Castelijn,
R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen,
C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu, MC and Chudoba, J},
Title = {Combination of Searches for Invisible Higgs Boson Decays
with the ATLAS Experiment.},
Journal = {Physical review letters},
Volume = {122},
Number = {23},
Pages = {231801},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.122.231801},
Abstract = {Dark matter particles, if sufficiently light, may be
produced in decays of the Higgs boson. This Letter presents
a statistical combination of searches for H→invisible
decays where H is produced according to the standard model
via vector boson fusion, Z(ℓℓ)H, and W/Z(had)H, all
performed with the ATLAS detector using 36.1 fb^{-1} of
pp collisions at a center-of-mass energy of
sqrt[s]=13 TeV at the LHC. In combination with the
results at sqrt[s]=7 and 8 TeV, an exclusion limit on the
H→invisible branching ratio of 0.26(0.17_{-0.05}^{+0.07})
at 95% confidence level is observed (expected).},
Doi = {10.1103/physrevlett.122.231801},
Key = {fds347443}
}
@article{fds307580,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Combination of searches for the Higgs boson using the full
CDF data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.88.052013},
Abstract = {We present a combination of searches for the standard model
Higgs boson using the full CDF run II data set, which
corresponds to an integrated luminosity of 9.45-10.0 fb-1
collected from √s=1.96 TeV pp̄ collisions at the Fermilab
Tevatron. The searches consider Higgs boson production from
gluon-gluon fusion, vector-boson fusion, and associated
production with either a W or Z boson or a tt̄ pair.
Depending on the production mode, Higgs boson decays to
W+W-, ZZ, bb̄, τ+τ-, and γγ are examined. We search for
a Higgs boson with masses (mH) in the range 90-200 GeV/c2.
In the absence of a signal, we expect based on combined
search sensitivity to exclude at the 95% credibility level
the mass regions 90<mH<94 GeV/c2, 96<mH<106 GeV/c2, and
153<mH<175 GeV/c2. The observed exclusion regions are
90<mH<102 GeV/c2 and 149<mH<172 GeV/c2. A moderate excess of
signal-like events relative to the background expectation at
the level of 2.0 standard deviations is present in the data
for the mH=125 GeV/c2 search hypothesis. We also present
interpretations of the data within the context of a
fermiophobic model and an alternative standard model
incorporating a fourth generation of fermions. Finally, for
the hypothesis of a new particle with mass 125 GeV/c2, we
constrain the coupling strengths of the new particle to W±
bosons, Z bosons, and fermions. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.052013},
Key = {fds307580}
}
@article{fds356772,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Combination of searches for WW, WZ, and ZZ resonances in pp
collisions at √s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {755},
Pages = {285-305},
Year = {2016},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2016.02.015},
Abstract = {The ATLAS experiment at the CERN Large Hadron Collider has
performed searches for new, heavy bosons decaying to WW, WZ
and ZZ final states in multiple decay channels using 20.3
fb−1 of pp collision data at s=8 TeV. In the current
study, the results of these searches are combined to provide
a more stringent test of models predicting heavy resonances
with couplings to vector bosons. Direct searches for a
charged diboson resonance decaying to WZ in the
ℓνℓ′ℓ′ (ℓ=μ,e), ℓℓqq¯ ℓνqq¯ and fully
hadronic final states are combined and upper limits on the
rate of production times branching ratio to the WZ bosons
are compared with predictions of an extended gauge model
with a heavy W′ boson. In addition, direct searches for a
neutral diboson resonance decaying to WW and ZZ in the
ℓℓqq¯ ℓνqq¯ and fully hadronic final states are
combined and upper limits on the rate of production times
branching ratio to the WW and ZZ bosons are compared with
predictions for a heavy, spin-2 graviton in an extended
Randall–Sundrum model where the Standard Model fields are
allowed to propagate in the bulk of the extra
dimension.},
Doi = {10.1016/j.physletb.2016.02.015},
Key = {fds356772}
}
@article{fds307911,
Author = {Aaltonen, and T, and others},
Title = {Combination of Tevatron searches for the standard model
Higgs boson in the $W^+W^-$ decay mode},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {6},
Pages = {061802},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.061802},
Abstract = {http://arxiv.org/abs/1001.4162},
Doi = {10.1103/PhysRevLett.104.061802},
Key = {fds307911}
}
@article{fds347456,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines,
JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi
Gupta, D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee,
S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall,
A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi, RMB and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black,
JE and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, V and Buschmann, E and Bussey,
P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera
Urbán, S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace,
N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili,
B and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen,
S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng,
HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D},
Title = {Combination of the Searches for Pair-Produced Vectorlike
Partners of the Third-Generation Quarks at
sqrt[s]=13 TeV with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {121},
Number = {21},
Pages = {211801},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.121.211801},
Abstract = {A combination of the searches for pair-produced vectorlike
partners of the top and bottom quarks in various decay
channels (T→Zt/Wb/Ht, B→Zb/Wt/Hb) is performed using
36.1 fb^{-1} of pp collision data at
sqrt[s]=13 TeV with the ATLAS detector at the Large
Hadron Collider. The observed data are found to be in good
agreement with the standard model background prediction in
all individual searches. Therefore, combined
95% confidence-level upper limits are set on the production
cross section for a range of vectorlike quark scenarios,
significantly improving upon the reach of the individual
searches. Model-independent limits are set assuming the
vectorlike quarks decay to standard model particles. A
singlet T is excluded for masses below 1.31 TeV and a
singlet B is excluded for masses below 1.22 TeV. Assuming a
weak isospin (T,B) doublet and |V_{Tb}|≪|V_{tB}|, T and B
masses below 1.37 TeV are excluded.},
Doi = {10.1103/physrevlett.121.211801},
Key = {fds347456}
}
@article{fds307694,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori,
L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett,
K},
Title = {Combination of the top-quark mass measurements from the
Tevatron collider},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {9},
Pages = {092003},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.86.092003},
Abstract = {The top quark is the heaviest known elementary particle,
with a mass about 40 times larger than the mass of its
isospin partner, the bottom quark. It decays almost 100% of
the time to a W boson and a bottom quark. Using top-antitop
pairs at the Tevatron proton-antiproton collider, the CDF
and D0 Collaborations have measured the top quark's mass in
different final states for integrated luminosities of up to
5.8fb-1. This paper reports on a combination of these
measurements that results in a more precise value of the
mass than any individual decay channel can provide. It
describes the treatment of the systematic uncertainties and
their correlations. The mass value determined is
173.18±0.56(stat)±0.75(syst)GeV or 173.18±0.94GeV, which
has a precision of ±0.54%, making this the most precise
determination of the top-quark mass. © 2012 American
Physical Society.},
Doi = {10.1103/PhysRevD.86.092003},
Key = {fds307694}
}
@article{fds352490,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abou Zeid and OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and AlKhoury, K and Alberghi,
GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri,
AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Combination of the W boson polarization measurements in top
quark decays using ATLAS and CMS data at √s = 8
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {8},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2020)051},
Abstract = {The combination of measurements of the W boson polarization
in top quark decays performed by the ATLAS and CMS
collaborations is presented. The measurements are based on
proton-proton collision data produced at the LHC at a
centre-of-mass energy of 8 TeV, and corresponding to an
integrated luminosity of about 20 fb−1 for each
experiment. The measurements used events containing one
lepton and having different jet multiplicities in the final
state. The results are quoted as fractions of W bosons with
longitudinal (F0), left-handed (FL), or right-handed (FR)
polarizations. The resulting combined measurements of the
polarization fractions are F0 = 0.693 ± 0.014 and FL =
0.315 ± 0.011. The fraction FR is calculated from the
unitarity constraint to be FR = −0.008 ± 0.007. These
results are in agreement with the standard model predictions
at next-to-next-to-leading order in perturbative quantum
chromodynamics and represent an improvement in precision of
25 (29)% for F0 (FL) with respect to the most precise single
measurement. A limit on anomalous right-handed vector (VR),
and left- and right-handed tensor (gL, gR) tWb couplings is
set while fixing all others to their standard model values.
The allowed regions are [−0.11, 0.16] for VR, [−0.08,
0.05] for gL, and [−0.04, 0.02] for gR, at 95% confidence
level. Limits on the corresponding Wilson coefficients are
also derived. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP08(2020)051},
Key = {fds352490}
}
@article{fds356603,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras,
D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V},
Title = {Combinations of single-top-quark production cross-section
measurements and},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2019)088},
Abstract = {This paper presents the combinations of single-top-quark
production cross-section measurements by the ATLAS and CMS
Collaborations, using data from LHC proton-proton collisions
at s = 7 and 8 TeV corresponding to integrated luminosities
of 1.17 to 5.1 fb−1 at s = 7 TeV and 12.2 to 20.3 fb−1
at s = 8 TeV. These combinations are performed per
centre-of-mass energy and for each production mode:
t-channel, tW, and s-channel. The combined t-channel
cross-sections are 67.5 ± 5.7 pb and 87.7 ± 5.8 pb at s =
7 and 8 TeV respectively. The combined tW cross-sections are
16.3 ± 4.1 pb and 23.1 ± 3.6 pb at s = 7 and 8 TeV
respectively. For the s-channel cross-section, the
combination yields 4.9 ± 1.4 pb at s = 8 TeV. The square of
the magnitude of the CKM matrix element Vtb multiplied by a
form factor fLV is determined for each production mode and
centre-of-mass energy, using the ratio of the measured
cross-section to its theoretical prediction. It is assumed
that the top-quark-related CKM matrix elements obey the
relation |Vtd|, |Vts| ≪ |Vtb|. All the |fLVVtb|2
determinations, extracted from individual ratios at s = 7
and 8 TeV, are combined, resulting in |fLVVtb| = 1.02 ±
0.04 (meas.) ± 0.02 (theo.). All combined measurements are
consistent with their corresponding Standard Model
predictions.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP05(2019)088},
Key = {fds356603}
}
@article{fds356709,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Aushev, V and Aushev, Y and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brochmann,
M and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapelain,
A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou,
M-C and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and Cuth, J and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de Barbaro, P and de Jong, SJ and De La
Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov, SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto, F and Di Canto and A and Di Ruzza,
B and Diehl, HT and Diesburg, M and Ding, PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti,
A and Drutskoy, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison,
J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, A and Evdokimov, VN and Farrington, S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franc, J and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov,
V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr,
RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays,
C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich,
I and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr,
T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon,
K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour,
J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega,
J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R},
Title = {Combined Forward-Backward Asymmetry Measurements in
Top-Antitop Quark Production at the Tevatron.},
Journal = {Physical review letters},
Volume = {120},
Number = {4},
Pages = {042001},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.120.042001},
Abstract = {The CDF and D0 experiments at the Fermilab Tevatron have
measured the asymmetry between yields of forward- and
backward-produced top and antitop quarks based on their
rapidity difference and the asymmetry between their decay
leptons. These measurements use the full data sets collected
in proton-antiproton collisions at a center-of-mass energy
of sqrt[s]=1.96 TeV. We report the results of
combinations of the inclusive asymmetries and their
differential dependencies on relevant kinematic quantities.
The combined inclusive asymmetry is A_{FB}^{tt[over
¯]}=0.128±0.025. The combined inclusive and differential
asymmetries are consistent with recent standard model
predictions.},
Doi = {10.1103/physrevlett.120.042001},
Key = {fds356709}
}
@article{fds356637,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Combined measurement of differential and total cross
sections in the H → γγ and the H → ZZ⁎ → 4ℓ
decay channels at s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {786},
Pages = {114-133},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2018.09.019},
Abstract = {A combined measurement of differential and inclusive total
cross sections of Higgs boson production is performed using
36.1 fb−1 of 13 TeV proton–proton collision data
produced by the LHC and recorded by the ATLAS detector in
2015 and 2016. Cross sections are obtained from measured
H→γγ and H→ZZ⁎→4ℓ event yields, which are
combined taking into account detector efficiencies,
resolution, acceptances and branching fractions. The total
Higgs boson production cross section is measured to be
57.0−5.9+6.0 (stat.) −3.3+4.0 (syst.) pb, in agreement
with the Standard Model prediction. Differential
cross-section measurements are presented for the Higgs boson
transverse momentum distribution, Higgs boson rapidity,
number of jets produced together with the Higgs boson, and
the transverse momentum of the leading jet. The results from
the two decay channels are found to be compatible, and their
combination agrees with the Standard Model
predictions.},
Doi = {10.1016/j.physletb.2018.09.019},
Key = {fds356637}
}
@article{fds375227,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arbiol
Val, SJ and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni,
G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Baer, TM and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beaucamp, JY and Beauchemin, PH and Becherer, F and Bechtle, P and Beck,
HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berrocal Guardia and A and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto, D and Boscherini,
D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton,
D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost,
E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos,
F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM},
Title = {Combined Measurement of the Higgs Boson Mass from the
H→γγ and H→ZZ^{*}→4ℓ Decay Channels with the ATLAS
Detector Using sqrt[s]=7, 8, and 13 TeV pp Collision
Data.},
Journal = {Physical review letters},
Volume = {131},
Number = {25},
Pages = {251802},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.131.251802},
Abstract = {A measurement of the mass of the Higgs boson combining the
H→ZZ^{*}→4ℓ and H→γγ decay channels is presented.
The result is based on 140 fb^{-1} of proton-proton
collision data collected by the ATLAS detector during LHC
run 2 at a center-of-mass energy of 13 TeV combined with
the run 1 ATLAS mass measurement, performed at
center-of-mass energies of 7 and 8 TeV, yielding a Higgs
boson mass of 125.11±0.09(stat)±0.06(syst)=125.11±0.11 GeV.
This corresponds to a 0.09% precision achieved on this
fundamental parameter of the Standard Model of particle
physics.},
Doi = {10.1103/physrevlett.131.251802},
Key = {fds375227}
}
@article{fds310284,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
Title = {Combined Measurement of the Higgs Boson Mass in pp
Collisions at sqrt[s]=7 and 8 TeV with the ATLAS and CMS
Experiments.},
Journal = {Physical review letters},
Volume = {114},
Number = {19},
Pages = {191803},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.114.191803},
Abstract = {A measurement of the Higgs boson mass is presented based on
the combined data samples of the ATLAS and CMS experiments
at the CERN LHC in the H→γγ and H→ZZ→4ℓ decay
channels. The results are obtained from a simultaneous fit
to the reconstructed invariant mass peaks in the two
channels and for the two experiments. The measured masses
from the individual channels and the two experiments are
found to be consistent among themselves. The combined
measured mass of the Higgs boson is m_{H}=125.09±0.21
(stat)±0.11 (syst) GeV.},
Doi = {10.1103/physrevlett.114.191803},
Key = {fds310284}
}
@article{fds356547,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Akesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Alvarez Piqueras and D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Combined measurements of Higgs boson production and decay
using up to 80 fb-1 of proton-proton collision
data at √s =13 TeV collected with the ATLAS
experiment},
Journal = {Physical Review D},
Volume = {101},
Number = {1},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.101.012002},
Abstract = {Combined measurements of Higgs boson production cross
sections and branching fractions are presented. The
combination is based on the analyses of the Higgs boson
decay modes H → γγ, ZZ∗, WW∗, τ τ, bb, μ μ,
searches for decays into invisible final states, and on
measurements of off-shell Higgs boson production. Up to 79.8
fb-1 of proton-proton collision data collected at √ = 13
TeV with the ATLAS detector are used. Results are presented
for the gluon-gluon fusion and vector-boson fusion
processes, and for associated production with vector bosons
or top-quarks. The global signal strength is determined to
be μ = 1.11-0.08+0.09. The combined measurement yields an
observed (expected) significance for the vector-boson fusion
production process of 6.5δ (5.3δ). Measurements in
kinematic regions defined within the simplified template
cross section framework are also shown. The results are
interpreted in terms of modifiers applied to the Standard
Model couplings of the Higgs boson to other particles, and
are used to set exclusion limits on parameters in
two-Higgs-doublet models and in the simplified minimal
supersymmetric Standard Model. No significant deviations
from Standard Model predictions are observed.},
Doi = {10.1103/PhysRevD.101.012002},
Key = {fds356547}
}
@article{fds310403,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jindariani, S and Jones,
M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi,
A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Tipton, P and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund,
AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Combined search for the standard model Higgs boson decaying
to a bb pair using the full CDF data set.},
Journal = {Physical review letters},
Volume = {109},
Number = {11},
Pages = {111802},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.109.111802},
Abstract = {We combine the results of searches for the standard model
(SM) Higgs boson based on the full CDF Run II data set
obtained from sqrt[s]=1.96 TeV pp collisions at the
Fermilab Tevatron corresponding to an integrated luminosity
of 9.45 fb(-1). The searches are conducted for Higgs
bosons that are produced in association with a W or Z boson,
have masses in the range 90-150 GeV/c(2), and decay
into bb pairs. An excess of data is present that is
inconsistent with the background prediction at the level of
2.5 standard deviations (the most significant local excess
is 2.7 standard deviations).},
Doi = {10.1103/physrevlett.109.111802},
Key = {fds310403}
}
@article{fds307720,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Combined search for the Standard Model Higgs boson in pp
collisions at √s=7TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.032003},
Abstract = {A combined search for the Standard Model Higgs boson with
the ATLAS detector at the LHC is presented. The data sets
used correspond to integrated luminosities from 4.6fb-1 to
4.9fb-1 of proton-proton collisions collected at √s=7TeV
in 2011. The Higgs boson mass ranges of 111.4 GeV to 116.6
GeV, 119.4 GeV to 122.1 GeV, and 129.2 GeV to 541 GeV are
excluded at the 95% confidence level, while the range 120
GeV to 560 GeV is expected to be excluded in the absence of
a signal. An excess of events is observed at Higgs boson
mass hypotheses around 126 GeV with a local significance of
2.9 standard deviations (σ). The global probability for the
background to produce an excess at least as significant
anywhere in the entire explored Higgs boson mass range of
110-600 GeV is estimated to be ∼15%, corresponding to a
significance of approximately 1σ. © 2012
CERN.},
Doi = {10.1103/PhysRevD.86.032003},
Key = {fds307720}
}
@article{fds307778,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Combined search for the Standard Model Higgs boson using up
to 4.9 fb-1 of pp collision data at s=7TeV with
the ATLAS detector at the LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {710},
Number = {1},
Pages = {49-66},
Publisher = {Elsevier BV},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2012.02.044},
Abstract = {A combined search for the Standard Model Higgs boson with
the ATLAS experiment at the LHC using datasets corresponding
to integrated luminosities from 1.04 fb-1 to 4.9 fb-1 of pp
collisions collected at s=7TeV is presented. The Higgs boson
mass ranges 112.9-115.5 GeV, 131-238 GeV and 251-466 GeV are
excluded at the 95% confidence level (CL), while the range
124-519 GeV is expected to be excluded in the absence of a
signal. An excess of events is observed around mH~126GeV
with a local significance of 3.5 standard deviations (σ).
The local significances of H→γγ, H→ZZ(z.ast;)→ℓ+ℓ-ℓ'+ℓ'-
and H→WW(z.ast;)→ℓ+νℓ'-ν- the three most sensitive
channels in this mass range, are 2.8σ, 2.1σ and 1.4σ,
respectively. The global probability for the background to
produce such a fluctuation anywhere in the explored Higgs
boson mass range 110-600 GeV is estimated to be ~1.4% or,
equivalently, 2.2σ. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.02.044},
Key = {fds307778}
}
@article{fds307914,
Author = {Aaltonen, and T, and others},
Title = {Combined Tevatron upper limit on $gg\rightarrow{}H\rightarrow{}W^{+}W^{-}$
and constraints on the Higgs boson mass in fourth-generation
fermion models},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {1},
Pages = {011102},
Publisher = {American Physical Society},
Year = {2010},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.82.011102},
Abstract = {We combine results from searches by the CDF and D0
collaborations for a standard model Higgs boson (H) in the
process gg→H→W+W - in pp̄ collisions at the Fermilab
Tevatron Collider at √s=1.96TeV. With 4.8fb-1 of
integrated luminosity analyzed at CDF and 5.4fb-1 at D0, the
95% confidence level upper limit on σ(gg→H)×B(H→W+W-)
is 1.75 pb at mH=120GeV, 0.38 pb at mH=165GeV, and 0.83 pb
at mH=200GeV. Assuming the presence of a fourth sequential
generation of fermions with large masses, we exclude at the
95% confidence level a standard-model-like Higgs boson with
a mass between 131 and 204 GeV. © 2010 The American
Physical Society.},
Doi = {10.1103/PhysRevD.82.011102},
Key = {fds307914}
}
@article{fds346216,
Author = {Seth, T and Kotwal, A and Thakur, R and Singh, P and Kochupillai,
V},
Title = {Common cancers in India: knowledge, attitudes and behaviours
of urban slum dwellers in New Delhi.},
Journal = {Public health},
Volume = {119},
Number = {2},
Pages = {87-96},
Year = {2005},
Month = {February},
url = {http://dx.doi.org/10.1016/j.puhe.2004.05.013},
Abstract = {<h4>Research questions</h4>What is the level of knowledge
and awareness of common cancers? What are the prevalent
attitudes and behaviours relating to common
cancers?<h4>Objectives</h4>To assess knowledge, attitudes
and behaviours regarding common cancers amongst urban slum
dwellers in New Delhi.<h4>Study design</h4>Field-based
cross-sectional survey of an urban slum cluster.<h4>Setting</h4>Slum
clusters along Pankha Road, West New Delhi.<h4>Participants</h4>Slum
dwellers of selected slums.<h4>Study variables</h4>Independent
variables were sociodemographic factors. Dependent variables
were knowledge, attitudes and behaviours regarding
preventive and curative aspects of common
cancers.<h4>Statistical analysis</h4>Proportions, confidence
intervals, tests of significance and multiple logistic
regression.<h4>Results</h4>Only 13% (10.6-15.7%) of the
study participants were aware of Pap smears, and only 2%
(1.1-3.3%) were able to identify all the common signs of
cancer. However, 87% (84.4-89.5%) of the study participants
knew that tobacco is a risk factor for cancer. Overall, 51%
(47.2-54.7%) had some knowledge pertaining to
cancer.<h4>Conclusion</h4>A focused, concerted and effective
information, education and communication drive is urgently
needed for all aspects of common cancers in
India.},
Doi = {10.1016/j.puhe.2004.05.013},
Key = {fds346216}
}
@article{fds347537,
Author = {Vasilopoulos, T and Kotwal, A and Huisingh-Scheetz, MJ and Waite, LJ and McClintock, MK and Dale, W},
Title = {Comorbidity and chronic conditions in the National Social
Life, Health and Aging Project (NSHAP), Wave
2.},
Journal = {The journals of gerontology. Series B, Psychological
sciences and social sciences},
Volume = {69 Suppl 2},
Pages = {S154-S165},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1093/geronb/gbu025},
Abstract = {<h4>Objective</h4>The goals of this paper were: (a) to
promote research using the National Social Life, Health and
Aging Project (NSHAP) Wave 2 data by providing relevant
background information for a broad range of chronic
conditions and (b) to provide a framework for combining
these chronic conditions into informative comorbidity
indices.<h4>Method</h4>The chronic conditions measured in
NSHAP Wave 2 were grouped across several health domains:
cardiovascular, endocrine and metabolic, cancer, lung,
inflammatory and bone, neurological, and sensorimotor.
Prevalences for each condition were reported as percentages
and were also estimated separately by age group and gender.
Additionally, 2 comorbidity indices were created: a Modified
Charlson Comorbidity Index (CCI) that included conditions
associated with mortality risk and the NSHAP Comorbidity
Index (NCI) that included conditions from the Modified CCI
as well as additional conditions related to overall health
and function.<h4>Results</h4>Hypertension, incontinence,
arthritis, heart conditions, cancer, and diabetes were the
most prevalent conditions. In general, prevalences of most
chronic conditions increased with age. Additionally, there
were several notable gender differences in chronic condition
prevalence. Due to the inclusion of highly prevalent
conditions, such as hypertension and incontinence, the mean
comorbidity index score of the NCI was higher than that of
the Modified CCI.<h4>Discussion</h4>Wave 2 of NSHAP included
a variety of measures assessing the chronic conditions that
are the most prevalent in older adults. These data are a
valuable resource for the study of the impact of chronic
conditions on overall health and aging.},
Doi = {10.1093/geronb/gbu025},
Key = {fds347537}
}
@article{fds356633,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
H},
Title = {Comparison between simulated and observed LHC beam
backgrounds in the ATLAS experiment at E beam =4
TeV},
Journal = {Journal of Instrumentation},
Volume = {13},
Number = {12},
Year = {2018},
Month = {December},
url = {http://dx.doi.org/10.1088/1748-0221/13/12/P12006},
Abstract = {Results of dedicated Monte Carlo simulations of beam-induced
background (BIB) in the ATLAS experiment at the Large Hadron
Collider (LHC) are presented and compared with data recorded
in 2012. During normal physics operation this background
arises mainly from scattering of the 4 TeV protons on
residual gas in the beam pipe. Methods of reconstructing the
BIB signals in the ATLAS detector, developed and implemented
in the simulation chain based on the \textsc{Fluka} Monte
Carlo simulation package, are described. The interaction
rates are determined from the residual gas pressure
distribution in the LHC ring in order to set an absolute
scale on the predicted rates of BIB so that they can be
compared quantitatively with data. Through these comparisons
the origins of the BIB leading to different observables in
the ATLAS detectors are analysed. The level of agreement
between simulation results and BIB measurements by ATLAS in
2012 demonstrates that a good understanding of the origin of
BIB has been reached.},
Doi = {10.1088/1748-0221/13/12/P12006},
Key = {fds356633}
}
@article{fds347183,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V},
Title = {Comparison of Fragmentation Functions for Jets Dominated by
Light Quarks and Gluons from pp and Pb+Pb Collisions in
ATLAS.},
Journal = {Physical review letters},
Volume = {123},
Number = {4},
Pages = {042001},
Year = {2019},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.123.042001},
Abstract = {Charged-particle fragmentation functions for jets
azimuthally balanced by a high-transverse-momentum, prompt,
isolated photon are measured in 25 pb^{-1} of pp and
0.49 nb^{-1} of Pb+Pb collision data at 5.02 TeV per
nucleon pair recorded with the ATLAS detector at the Large
Hadron Collider. The measurements are compared to
predictions of Monte Carlo generators and to measurements
of inclusively selected jets. In pp collisions, a different
jet fragmentation function in photon-tagged events from that
in inclusive jet events arises from the difference in
fragmentation between light quarks and gluons. The ratios of
the fragmentation functions in Pb+Pb events to that in pp
events are used to explore the parton color-charge
dependence of jet quenching in the hot medium. In relatively
peripheral collisions, fragmentation functions exhibit a
similar modification pattern for photon-tagged and inclusive
jets. However, photon-tagged jets are observed to have
larger modifications than inclusive jets in central Pb+Pb
events.},
Doi = {10.1103/physrevlett.123.042001},
Key = {fds347183}
}
@article{fds313622,
Author = {Kotwal, AV and Jayatilaka, B},
Title = {Comparison of HORACE and PHOTOS algorithms for multiphoton
emission in the context of W boson mass measurement},
Journal = {Advances in High Energy Physics},
Volume = {2016},
Number = {1615081},
Pages = {1-9},
Publisher = {Hindawi Limited},
Year = {2016},
Month = {January},
ISSN = {1687-7357},
url = {http://dx.doi.org/10.1155/2016/1615081},
Abstract = {W boson mass measurement is sensitive to QED radiative
corrections due to virtual photon loops and real photon
emission. The largest shift in the measured mass, which
depends on the transverse momentum spectrum of the charged
lepton from the boson decay, is caused by the emission of
real photons from the final-state lepton. There are a number
of calculations and codes available to model the final-state
photon emission. We perform a detailed study, comparing the
results from horace and photos implementations of the
final-state multiphoton emission in the context of a direct
measurement of W boson mass at Tevatron. Mass fits are
performed using a simulation of the CDF II
detector.},
Doi = {10.1155/2016/1615081},
Key = {fds313622}
}
@article{fds373066,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Comparison of inclusive and photon-tagged jet suppression in
5.02 TeV Pb+Pb collisions with ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {846},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138154},
Abstract = {Parton energy loss in the quark–gluon plasma (QGP) is
studied with a measurement of photon-tagged jet production
in 1.7 nb−1 of Pb+Pb data and 260 pb−1 of pp data, both
at sNN=5.02 TeV, with the ATLAS detector. The process pp
→γ+jet+X and its analogue in Pb+Pb collisions is measured
in events containing an isolated photon with transverse
momentum (pT) above 50 GeV and reported as a function of jet
pT. This selection results in a sample of jets with a
steeply falling pT distribution that are mostly initiated by
the showering of quarks. The pp and Pb+Pb measurements are
used to report the nuclear modification factor, RAA, and the
fractional energy loss, Sloss, for photon-tagged jets. In
addition, the results are compared with the analogous ones
for inclusive jets, which have a significantly smaller
quark-initiated fraction. The RAA and Sloss values are found
to be significantly different between those for
photon-tagged jets and inclusive jets, demonstrating that
energy loss in the QGP is sensitive to the colour-charge of
the initiating parton. The results are also compared with a
variety of theoretical models of colour-charge-dependent
energy loss.},
Doi = {10.1016/j.physletb.2023.138154},
Key = {fds373066}
}
@article{fds310337,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Comprehensive measurements of t-channel single top-quark
production cross sections at √s=7 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.112006},
Abstract = {This article presents measurements of the t-channel single
top-quark (t) and top-antiquark (t¯) total production cross
sections σ(tq) and σ(t¯q), their ratio
Rt=σ(tq)/σ(t¯q), and a measurement of the inclusive
production cross section σ(tq+t¯q) in proton-proton
collisions at √s=7 TeV at the LHC. Differential cross
sections for the tq and t¯q processes are measured as a
function of the transverse momentum and the absolute value
of the rapidity of t and t¯, respectively. The analyzed
data set was recorded with the ATLAS detector and
corresponds to an integrated luminosity of 4.59 fb-1.
Selected events contain one charged lepton, large missing
transverse momentum, and two or three jets. The cross
sections are measured by performing a binned
maximum-likelihood fit to the output distributions of neural
networks. The resulting measurements are
σ(tq)=46±1(stat)±6(syst) pb, σ(t¯q)=23±1(stat)±3(syst)
pb, Rt=2.04±0.13(stat)±0.12(syst), and
σ(tq+t¯q)=68±2(stat)±8(syst) pb, consistent with the
Standard Model expectation. The uncertainty on the measured
cross sections is dominated by systematic uncertainties,
while the uncertainty on Rt is mainly statistical. Using the
ratio of σ(tq+t¯q) to its theoretical prediction, and
assuming that the top-quark-related CKM matrix elements obey
the relation |Vtb||Vts|,|Vtd|, we determine
|Vtb|=1.02±0.07.},
Doi = {10.1103/PhysRevD.90.112006},
Key = {fds310337}
}
@article{fds360566,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alison, J and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Aranzabal, N and Araujo Ferraz and V and Pereira, RA and Arcangeletti, C and Arce, ATH},
Title = {Configuration and performance of the ATLAS b-jet triggers in
Run 2},
Journal = {European Physical Journal C},
Volume = {81},
Number = {12},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09775-5},
Abstract = {Several improvements to the ATLAS triggers used to identify
jets containing b-hadrons (b-jets) were implemented for
data-taking during Run 2 of the Large Hadron Collider from
2016 to 2018. These changes include reconfiguring the b-jet
trigger software to improve primary-vertex finding and allow
more stable running in conditions with high pile-up, and the
implementation of the functionality needed to run
sophisticated taggers used by the offline reconstruction in
an online environment. These improvements yielded an order
of magnitude better light-flavour jet rejection for the same
b-jet identification efficiency compared to the performance
in Run 1 (2011–2012). The efficiency to identify b-jets
in the trigger, and the conditional efficiency for b-jets
that satisfy offline b-tagging requirements to pass the
trigger are also measured. Correction factors are derived to
calibrate the b-tagging efficiency in simulation to match
that observed in data. The associated systematic
uncertainties are substantially smaller than in previous
measurements. In addition, b-jet triggers were operated for
the first time during heavy-ion data-taking, using dedicated
triggers that were developed to identify semileptonic
b-hadron decays by selecting events with geometrically
overlapping muons and jets.},
Doi = {10.1140/epjc/s10052-021-09775-5},
Key = {fds360566}
}
@article{fds364959,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
Title = {Constraints on Higgs boson properties using
WW∗(→ eνμν) jj production in
36.1fb-1 of √s=13 TeV pp collisions with the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {7},
Year = {2022},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10366-1},
Abstract = {This article presents the results of two studies of Higgs
boson properties using the WW∗(→ eνμν) jj final
state, based on a dataset corresponding to 36.1 fb - 1 of
s=13 TeV proton–proton collisions recorded by the ATLAS
experiment at the Large Hadron Collider. The first study
targets Higgs boson production via gluon–gluon fusion and
constrains the CP properties of the effective Higgs–gluon
interaction. Using angular distributions and the overall
rate, a value of tan (α) = 0.0 ± 0.4 (stat.) ± 0.3
(syst.) is obtained for the tangent of the mixing angle for
CP-even and CP-odd contributions. The second study exploits
the vector-boson fusion production mechanism to probe the
Higgs boson couplings to longitudinally and transversely
polarised W and Z bosons in both the production and the
decay of the Higgs boson; these couplings have not been
directly constrained previously. The polarisation-dependent
coupling-strength scale factors are defined as the ratios of
the measured polarisation-dependent coupling strengths to
those predicted by the Standard Model, and are determined
using rate and kinematic information to be
aL=0.91-0.18+0.10(stat.)-0.17+0.09(syst.) and aT= 1.2 ± 0.4
(stat.)-0.3+0.2(syst.). These coupling strengths are
translated into pseudo-observables, resulting in
κVV=0.91-0.18+0.10(stat.)-0.17+0.09(syst.) and
ϵVV=0.13-0.20+0.28 (stat.)-0.10+0.08(syst.). All results
are consistent with the Standard Model predictions.},
Doi = {10.1140/epjc/s10052-022-10366-1},
Key = {fds364959}
}
@article{fds356607,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Arduh, FA},
Title = {Constraints on mediator-based dark matter and scalar dark
energy models using √s = 13 TeV pp collision data
collected by the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2019)142},
Abstract = {Constraints on selected mediator-based dark matter models
and a scalar dark energy model using up to 37 fb−1s = 13
TeV pp collision data collected by the ATLAS detector at the
LHC during 2015-2016 are summarised in this paper. The
results of experimental searches in a variety of final
states are interpreted in terms of a set of spin-1 and
spin-0 single-mediator dark matter simplified models and a
second set of models involving an extended Higgs sector plus
an additional vector or pseudo-scalar mediator. The searches
considered in this paper constrain spin-1 leptophobic and
leptophilic mediators, spin-0 colour-neutral and
colour-charged mediators and vector or pseudo-scalar
mediators embedded in extended Higgs sector models. In this
case, also s = 8 TeV pp collision data are used for the
interpretation of the results. The results are also
interpreted for the first time in terms of light scalar
particles that could contribute to the accelerating
expansion of the universe (dark energy).[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP05(2019)142},
Key = {fds356607}
}
@article{fds310290,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn,
SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes,
RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori,
M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
L and Margaroli, F and Marino, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and (CDF
Collaboration)},
Title = {Constraints on models of the Higgs boson with exotic spin
and parity using decays to bottom-antibottom quarks in the
full CDF data set.},
Journal = {Physical review letters},
Volume = {114},
Number = {14},
Pages = {141802},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.114.141802},
Abstract = {A search for particles with the same mass and couplings as
those of the standard model Higgs boson but different spin
and parity quantum numbers is presented. We test two
specific alternative Higgs boson hypotheses: a pseudoscalar
Higgs boson with spin-parity J^{P}=0^{-} and a gravitonlike
Higgs boson with J^{P}=2^{+}, assuming for both a mass of
125 GeV/c^{2}. We search for these exotic states
produced in association with a vector boson and decaying
into a bottom-antibottom quark pair. The vector boson is
reconstructed through its decay into an electron or muon
pair, or an electron or muon and a neutrino, or it is
inferred from an imbalance in total transverse momentum. We
use expected kinematic differences between events containing
exotic Higgs bosons and those containing standard model
Higgs bosons. The data were collected by the CDF experiment
at the Tevatron proton-antiproton collider, operating at a
center-of-mass energy of sqrt[s]=1.96 TeV, and
correspond to an integrated luminosity of 9.45 fb^{-1}.
We exclude deviations from the predictions of the standard
model with a Higgs boson of mass 125 GeV/c^{2} at the
level of 5 standard deviations, assuming signal strengths
for exotic boson production equal to the prediction for the
standard model Higgs boson, and set upper limits of
approximately 30% relative to the standard model rate on the
possible rate of production of each exotic
state.},
Doi = {10.1103/physrevlett.114.141802},
Key = {fds310290}
}
@article{fds348986,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Constraints on new phenomena via Higgs boson couplings and
invisible decays with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {11},
Pages = {1-52},
Year = {2015},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2015)206},
Abstract = {Abstract: The ATLAS experiment at the LHC has measured the
Higgs boson couplings and mass, and searched for invisible
Higgs boson decays, using multiple production and decay
channels with up to 4.7 fb−1 of pp collision data at−1at
TeV. In the current study, the measured production and decay
rates of the observed Higgs boson in the γγ, ZZ, W W ,
Zγ, bb, τ τ , and μμ decay channels, along with results
from the associated production of a Higgs boson with a
top-quark pair, are used to probe the scaling of the
couplings with mass. Limits are set on parameters in
extensions of the Standard Model including a composite Higgs
boson, an additional electroweak singlet, and
two-Higgs-doublet models. Together with the measured mass of
the scalar Higgs boson in the γγ and ZZ decay modes, a
lower limit is set on the pseudoscalar Higgs boson mass of
mA> 370 GeV in the “hMSSM” simplified Minimal
Supersymmetric Standard Model. Results from direct searches
for heavy Higgs bosons are also interpreted in the hMSSM.
Direct searches for invisible Higgs boson decays in the
vector-boson fusion and associated production of a Higgs
boson with W/Z (Z → ℓℓ, W/Z → jj) modes are
statistically combined to set an upper limit on the Higgs
boson invisible branching ratio of 0.25. The use of the
measured visible decay rates in a more general coupling fit
improves the upper limit to 0.23, constraining a Higgs
portal model of dark matter.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP11(2015)206},
Key = {fds348986}
}
@article{fds356781,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Constraints on non-Standard Model Higgs boson interactions
in an effective Lagrangian using differential cross sections
measured in the H → γγ decay channel at √s=8 TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {753},
Pages = {69-85},
Year = {2016},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2015.11.071},
Abstract = {The strength and tensor structure of the Higgs boson's
interactions are investigated using an effective Lagrangian,
which introduces additional CP-even and CP-odd interactions
that lead to changes in the kinematic properties of the
Higgs boson and associated jet spectra with respect to the
Standard Model. The parameters of the effective Lagrangian
are probed using a fit to five differential cross sections
previously measured by the ATLAS experiment in the H→γγ
decay channel with an integrated luminosity of 20.3 fb−1
at s=8 TeV. In order to perform a simultaneous fit to the
five distributions, the statistical correlations between
them are determined by re-analysing the H→γγ candidate
events in the proton–proton collision data. No significant
deviations from the Standard Model predictions are observed
and limits on the effective Lagrangian parameters are
derived. The statistical correlations are made publicly
available to allow for future analysis of theories with
non-Standard Model interactions.},
Doi = {10.1016/j.physletb.2015.11.071},
Key = {fds356781}
}
@article{fds356640,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Constraints on off-shell Higgs boson production and the
Higgs boson total width in ZZ → 4ℓ and
ZZ → 2ℓ2ν final states with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {786},
Pages = {223-244},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2018.09.048},
Abstract = {A measurement of off-shell Higgs boson production in the
ZZ→4ℓ and ZZ→2ℓ2ν decay channels, where ℓ stands
for either an electron or a muon, is performed using data
from proton–proton collisions at a centre-of-mass energy
of s=13 TeV. The data were collected by the ATLAS experiment
in 2015 and 2016 at the Large Hadron Collider, and they
correspond to an integrated luminosity of 36.1fb−1. An
observed (expected) upper limit on the off-shell Higgs
signal strength, defined as the event yield normalised to
the Standard Model prediction, of 3.8 (3.4) is obtained at
95% confidence level (CL). Assuming the ratio of the Higgs
boson couplings to the Standard Model predictions is
independent of the momentum transfer of the Higgs production
mechanism considered in the analysis, a combination with the
on-shell signal-strength measurements yields an observed
(expected) 95% CL upper limit on the Higgs boson total width
of 14.4 (15.2) MeV.},
Doi = {10.1016/j.physletb.2018.09.048},
Key = {fds356640}
}
@article{fds371633,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Constraints on spin-0 dark matter mediators and invisible
Higgs decays using ATLAS 13 TeV pp collision data with two
top quarks and missing transverse momentum in the final
state},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11477-z},
Abstract = {This paper presents a statistical combination of searches
targeting final states with two top quarks and invisible
particles, characterised by the presence of zero, one or two
leptons, at least one jet originating from a b-quark and
missing transverse momentum. The analyses are searches for
phenomena beyond the Standard Model consistent with the
direct production of dark matter in pp collisions at the
LHC, using 139 fb - 1 of data collected with the ATLAS
detector at a centre-of-mass energy of 13 TeV. The results
are interpreted in terms of simplified dark matter models
with a spin-0 scalar or pseudoscalar mediator particle. In
addition, the results are interpreted in terms of upper
limits on the Higgs boson invisible branching ratio, where
the Higgs boson is produced according to the Standard Model
in association with a pair of top quarks. For scalar
(pseudoscalar) dark matter models, with all couplings set to
unity, the statistical combination extends the mass range
excluded by the best of the individual channels by
50 (25) GeV, excluding mediator masses up to 370 GeV. In
addition, the statistical combination improves the expected
coupling exclusion reach by 14% (24%), assuming a scalar
(pseudoscalar) mediator mass of 10 GeV. An upper limit on
the Higgs boson invisible branching ratio of 0.38
(0.30-0.09+0.13) is observed (expected) at 95% confidence
level.},
Doi = {10.1140/epjc/s10052-023-11477-z},
Key = {fds371633}
}
@article{fds372124,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Constraints on the Higgs boson self-coupling from single-
and double-Higgs production with the ATLAS detector using pp
collisions at s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137745},
Abstract = {Constraints on the Higgs boson self-coupling are set by
combining double-Higgs boson analyses in the bb¯bb¯,
bb¯τ+τ− and bb¯γγ decay channels with single-Higgs
boson analyses targeting the γγ, ZZ⁎, WW⁎, τ+τ−
and bb¯ decay channels. The data used in these analyses
were recorded by the ATLAS detector at the LHC in
proton–proton collisions at s=13 TeV and correspond to an
integrated luminosity of 126–139 fb−1. The combination
of the double-Higgs analyses sets an upper limit of μHH<2.4
at 95% confidence level on the double-Higgs production
cross-section normalised to its Standard Model prediction.
Combining the single-Higgs and double-Higgs analyses, with
the assumption that new physics affects only the Higgs boson
self-coupling (λHHH), values outside the interval
−0.4<κλ=(λHHH/λHHHSM)<6.3 are excluded at 95%
confidence level. The combined single-Higgs and double-Higgs
analyses provide results with fewer assumptions, by adding
in the fit more coupling modifiers introduced to account for
the Higgs boson interactions with the other Standard Model
particles. In this relaxed scenario, the constraint becomes
−1.4<κλ<6.1 at 95% CL.},
Doi = {10.1016/j.physletb.2023.137745},
Key = {fds372124}
}
@article{fds310330,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Constraints on the off-shell Higgs boson signal strength in
the high-mass ZZ and WW final states with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {335},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3542-2},
Abstract = {Measurements of the <i>ZZ</i> and <i>WW</i> final states in
the mass range above the [Formula: see text] and [Formula:
see text] thresholds provide a unique opportunity to measure
the off-shell coupling strength of the Higgs boson. This
paper presents constraints on the off-shell Higgs boson
event yields normalised to the Standard Model prediction
(signal strength) in the [Formula: see text], [Formula: see
text] and [Formula: see text] final states. The result is
based on <i>pp</i> collision data collected by the ATLAS
experiment at the LHC, corresponding to an integrated
luminosity of 20.3 fb[Formula: see text] at a collision
energy of [Formula: see text] TeV. Using the [Formula: see
text] method, the observed 95 [Formula: see text]
confidence level (CL) upper limit on the off-shell signal
strength is in the range 5.1-8.6, with an expected range of
6.7-11.0. In each case the range is determined by varying
the unknown [Formula: see text] and [Formula: see text]
background K-factor from higher-order quantum chromodynamics
corrections between half and twice the value of the known
signal K-factor. Assuming the relevant Higgs boson couplings
are independent of the energy scale of the Higgs boson
production, a combination with the on-shell measurements
yields an observed (expected) 95 [Formula: see text] CL
upper limit on [Formula: see text] in the range 4.5-7.5
(6.5-11.2) using the same variations of the background
K-factor. Assuming that the unknown [Formula: see text]
background K-factor is equal to the signal K-factor, this
translates into an observed (expected) 95 [Formula: see
text] CL upper limit on the Higgs boson total width of 22.7
(33.0) MeV.},
Doi = {10.1140/epjc/s10052-015-3542-2},
Key = {fds310330}
}
@article{fds329965,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Armitage, LJ},
Title = {Correction to: Identification and rejection of pile-up jets
at high pseudorapidity with the ATLAS detector (Eur. Phys.
J. C, (2017), 77, (580), 10.1140/epjc/s10052-017-5081-5)},
Journal = {European Physical Journal C},
Volume = {77},
Number = {10},
Publisher = {Springer Nature America, Inc},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5245-3},
Abstract = {Unfortunately, in the original version of this article the
copyright holder was wrong in the HTML. The original article
has been corrected.},
Doi = {10.1140/epjc/s10052-017-5245-3},
Key = {fds329965}
}
@article{fds356625,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Correlated long-range mixed-harmonic fluctuations measured
in pp, p+Pb and low-multiplicity Pb+Pb collisions with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {789},
Pages = {444-471},
Year = {2019},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2018.11.065},
Abstract = {Correlations of two flow harmonics vn and vm via three- and
four-particle cumulants are measured in 13 TeV pp, 5.02 TeV
p+Pb, and 2.76 TeV peripheral Pb+Pb collisions with the
ATLAS detector at the LHC. The goal is to understand the
multi-particle nature of the long-range collective
phenomenon in these collision systems. The large non-flow
background from dijet production present in the standard
cumulant method is suppressed using a method of subevent
cumulants involving two, three and four subevents separated
in pseudorapidity. The results show a negative correlation
between v2 and v3 and a positive correlation between v2 and
v4 for all collision systems and over the full multiplicity
range. However, the magnitudes of the correlations are found
to depend on the event multiplicity, the choice of
transverse momentum range and collision system. The relative
correlation strength, obtained by normalisation of the
cumulants with the 〈vn2〉 from a two-particle correlation
analysis, is similar in the three collision systems and
depends weakly on the event multiplicity and transverse
momentum. These results based on the subevent methods
provide strong evidence of a similar long-range
multi-particle collectivity in pp, p+Pb and peripheral Pb+Pb
collisions.},
Doi = {10.1016/j.physletb.2018.11.065},
Key = {fds356625}
}
@article{fds346214,
Author = {Kotwal, A and Thakur, R and Seth, T},
Title = {Correlates of tobacco-use pattern amongst adolescents in two
schools of New Delhi, India.},
Journal = {Indian journal of medical sciences},
Volume = {59},
Number = {6},
Pages = {243-252},
Year = {2005},
Month = {June},
url = {http://dx.doi.org/10.4103/0019-5359.16299},
Abstract = {<h4>Background</h4>As adolescent tobacco use has been found
to be a major predictor of future use, preventive efforts
need to be focused on this section of population.<h4>Objectives</h4>To
assess the role of knowledge regarding tobacco, risk-taking
attitude, peers, and other influencers on tobacco and areca
nut use, amongst adolescents.<h4>Settings and design</h4>A
school-based cross-sectional study covering two schools.
Students of classes IX and XI, of selected schools,
participated in the study (n = 596).<h4>Methods</h4>A
pretested and validated, close ended, self-administered
questionnaire was used. Sociodemographic factors, awareness
regarding tobacco, risk-taking attitudes, role of peers and
other influencers, and tobacco, areca nut and alcohol use,
were studied.<h4>Statistical analysis</h4>Point estimates,
98% Confidence Intervals, tests of significance, bivariate
and multivariate analysis (multiple logistic
regression).<h4>Results</h4>Almost 42% of tobacco users
started before the age of 12 years. Peer pressure, general
stress, and media were important influencers. Logistic
regression analysis showed that students in public school
were using more tobacco [Odds ratio (OR) = 1.85, P = 0.174]
and tobacco/areca nut (OR = 1.14, P = 0.02). The difference
in use between the genders and class in which studying was
statistically not significant. Lesser proportion of those
possessing adequate knowledge regarding tobacco used it as
compared to those without adequate knowledge (OR = 0.13, P <
0.001) however, possession of adequate knowledge was not a
good predictor of areca nut consumption (OR = 0.86, P =
0.585). The most important correlate for tobacco use (OR =
6.41, P < 0.001) and areca nut use (OR = 11.17, P < 0.001)
was risk-taking attitude.<h4>Conclusion</h4>Multi-pronged
and concerted efforts targeting children at an early age are
required to prevent tobacco and areca nut use among
adolescents.},
Doi = {10.4103/0019-5359.16299},
Key = {fds346214}
}
@article{fds346184,
Author = {Tiwari, M and Kotwal, J and Kotwal, A and Mishra, P and Dutta, V and Chopra, S},
Title = {Correlation of haemoglobin and red cell indices with serum
ferritin in Indian women in second and third trimester of
pregnancy.},
Journal = {Medical journal, Armed Forces India},
Volume = {69},
Number = {1},
Pages = {31-36},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.07.016},
Abstract = {<h4>Background</h4>Iron deficiency anaemia (IDA) is the most
common cause of anaemia in pregnancy in Indians and is
associated with increased risk of low birth-weight infants.
Studies from developed countries recommend iron
supplementation based on serum ferritin levels. However,
screening by serum ferritin is not feasible in all cases in
India. This study was undertaken to document haematological
profile of pregnant Indian women.<h4>Methods</h4>We studied
the correlation between second and third trimester ferritin
concentration and haemoglobin (Hb) and red cell indices in
100 consecutive ANC cases to select the best haematologic
characteristic to identify women who needed iron therapy. Hb
and red cell indices, RBC count, mean corpuscular volume,
mean corpuscular haemoglobin, mean corpuscular haemoglobin
concentration, red cell distribution width were analysed and
PBS studied to subtype anaemia if present.<h4>Results</h4>Proportion
of iron deficiency anaemia in pregnancy was 34% and
significant correlation was found between serum ferritin and
RDW-CV% and TRBC. No correlation was found between ferritin
levels and Hb, MCV, MCH and MCHC. Serum ferritin levels were
<12 ng/mL in 30 out of 52 non-anaemic cases suggesting
prevalence of sub-clinical iron deficiency in 58% cases.
None of the red cell indices correlated with ferritin level
in this group. Only TRBC showed some correlation with
ferritin (r = -0.090, p > 0.05).<h4>Conclusion</h4>All
pregnant women in India should continue to get iron
supplements unlike what is recommended in the developed
countries where iron supplementation is based on serum
ferritin levels.},
Doi = {10.1016/j.mjafi.2012.07.016},
Key = {fds346184}
}
@article{fds372392,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei,
D and Dos Santos and SPA and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Correlations between flow and transverse momentum in Xe + Xe
and Pb + Pb collisions at the LHC with the ATLAS detector: A
probe of the heavy-ion initial state and nuclear
deformation},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054910},
Abstract = {The correlations between flow harmonics vn for n = 2, 3, and
4 and mean transverse momentum [pT] in 129Xe + 129Xe and
208Pb + 208Pb collisions at √s = 5.44 and 5.02 TeV,
respectively, are measured using charged particles with the
ATLAS detector. The correlations are potentially sensitive
to the shape and size of the initial geometry, nuclear
deformation, and initial momentum anisotropy. The effects
from nonflow and centrality fluctuations are minimized,
respectively, via a subevent cumulant method and an
event-activity selection based on particle production at
very forward rapidity. The vn-[pT] correlations show strong
dependencies on centrality, harmonic number n, pT, and
pseudorapidity range. Current models qualitatively describe
the overall centrality- and system-dependent trends but fail
to quantitatively reproduce all features of the data. In
central collisions, where models generally show good
agreement, the v2-[pT] correlations are sensitive to the
triaxiality of the quadruple deformation. Comparison of the
model with the Pb + Pb and Xe + Xe data confirms that the
129Xe nucleus is a highly deformed triaxial ellipsoid that
has neither a prolate nor oblate shape. This provides strong
evidence for a triaxial deformation of the 129Xe nucleus
from high-energy heavy-ion collisions.},
Doi = {10.1103/PhysRevC.107.054910},
Key = {fds372392}
}
@article{fds351555,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asai,
K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou,
EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Besson,
N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona,
M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler,
S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
TM and Casado, MP and Casha, AF and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen,
J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chow, YS and Christopher, LD and Chu, MC and Chu, X},
Title = {CP Properties of Higgs Boson Interactions with Top Quarks in
the tt[over ¯]H and tH Processes Using H→γγ with the
ATLAS Detector.},
Journal = {Physical review letters},
Volume = {125},
Number = {6},
Pages = {061802},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.125.061802},
Abstract = {A study of the charge conjugation and parity (CP) properties
of the interaction between the Higgs boson and top quarks is
presented. Higgs bosons are identified via the diphoton
decay channel (H→γγ), and their production in
association with a top quark pair (tt[over ¯]H) or single
top quark (tH) is studied. The analysis uses
139 fb^{-1} of proton-proton collision data recorded at
a center-of-mass energy of sqrt[s]=13 TeV with the
ATLAS detector at the Large Hadron Collider. Assuming a
CP-even coupling, the tt[over ¯]H process is observed with
a significance of 5.2 standard deviations. The measured
cross section times H→γγ branching ratio is
1.64_{-0.36}^{+0.38}(stat)_{-0.14}^{+0.17}(sys) fb, and
the measured rate for tt[over ¯]H is 1.43_{-0.31}^{+0.33}(stat)_{-0.15}^{+0.21}(sys)
times the Standard Model expectation. The tH production
process is not observed and an upper limit on its rate of 12
times the Standard Model expectation is set. A CP-mixing
angle greater (less) than 43 (-43)° is excluded at
95% confidence level.},
Doi = {10.1103/physrevlett.125.061802},
Key = {fds351555}
}
@article{fds308208,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada,
J},
Title = {Cross section for b-jet production in supp¯p
collisions at √s=1.8 TeV},
Journal = {Physical Review Letters},
Volume = {85},
Number = {24},
Pages = {5068-5073},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.85.5068},
Abstract = {Bottom-quark production in p¯p collisions at √s=1.8 TeV
is studied with 5 pb−1 of data collected in 1995 by the D0
detector at the Fermilab Tevatron Collider. The differential
production cross section for b jets in the central rapidity
region (|yb|<1) as a function of jet transverse energy is
extracted from a muon-tagged jet sample. Within experimental
and theoretical uncertainties, D0 results are found to be
higher than, but compatible with, next-to-leading-order QCD
predictions. © 2000 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.85.5068},
Key = {fds308208}
}
@article{fds356609,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Cross-section measurements of the Higgs boson decaying into
a pair of τ -leptons in proton-proton collisions at s =13
TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {99},
Number = {7},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.99.072001},
Abstract = {A measurement of production cross sections of the Higgs
boson in proton-proton collisions is presented in the
H→ττ decay channel. The analysis is performed using 36.1
fb-1 of data recorded by the ATLAS experiment at the Large
Hadron Collider at a center-of-mass energy of s=13 TeV. All
combinations of leptonic (τ→vv with =e,μ) and hadronic
(τ→hadrons v) τ decays are considered. The H→ττ
signal over the expected background from other Standard
Model processes is established with an observed (expected)
significance of 4.4 (4.1) standard deviations. Combined with
results obtained using data taken at 7 and 8 TeV
center-of-mass energies, the observed (expected)
significance amounts to 6.4 (5.4) standard deviations and
constitutes an observation of H→ττ decays. Using the
data taken at s=13 TeV, the total cross section in the
H→ττ decay channel is measured to be 3.77-0.59+0.60
(stat) -0.74+0.87 (syst) pb, for a Higgs boson of mass 125
GeV assuming the relative contributions of its production
modes as predicted by the Standard Model. Total cross
sections in the H→ττ decay channel are determined
separately for vector-boson-fusion production and
gluon-gluon-fusion production to be σH→ττVBF=0.28±0.09
(stat) -0.09+0.11 (syst) pb and σH→ττggF=3.1±1.0
(stat) -1.3+1.6 (syst) pb, respectively. Similarly, results
of a fit are reported in the framework of simplified
template cross sections. All measurements are in agreement
with Standard Model expectations.},
Doi = {10.1103/PhysRevD.99.072001},
Key = {fds356609}
}
@article{fds346204,
Author = {Kotwal, A and Watt, D},
Title = {Cutaneous squamous cell carcinoma in a child.},
Journal = {Journal of plastic, reconstructive & aesthetic surgery :
JPRAS},
Volume = {62},
Number = {7},
Pages = {e194-e195},
Year = {2009},
Month = {July},
url = {http://dx.doi.org/10.1016/j.bjps.2009.03.008},
Abstract = {Cutaneous squamous cell carcinoma in children is very rare.
Of those reported cases, most arise in the context of
underlying predisposing conditions such as xeroderma
pigmentosum, albinism or immunosuppression. We report a rare
case of cutaneous squamous cell carcinoma in a child with no
history of predisposing conditions.},
Doi = {10.1016/j.bjps.2009.03.008},
Key = {fds346204}
}
@article{fds321098,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Dark matter interpretations of ATLAS searches for the
electroweak production of supersymmetric particles in √s=8
TeV proton-proton collisions},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)175},
Abstract = {A selection of searches by the ATLAS experiment at the LHC
for the electroweak production of SUSY particles are used to
study their impact on the constraints on dark matter
candidates. The searches use 20 fb−1 of proton-proton
collision data at s=8 TeV. A likelihood-driven scan of a
five-dimensional effective model focusing on the
gaugino-higgsino and Higgs sector of the phenomenological
minimal supersymmetric Standard Model is performed. This
scan uses data from direct dark matter detection
experiments, the relic dark matter density and precision
flavour physics results. Further constraints from the ATLAS
Higgs mass measurement and SUSY searches at LEP are also
applied. A subset of models selected from this scan are used
to assess the impact of the selected ATLAS searches in this
five-dimensional parameter space. These ATLAS searches
substantially impact those models for which the mass
m(χ˜10) of the lightest neutralino is less than 65 GeV,
excluding 86% of such models. The searches have limited
impact on models with larger m(χ˜10) due to either heavy
electroweakinos or compressed mass spectra where the mass
splittings between the produced particles and the lightest
supersymmetric particle is small.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP09(2016)175},
Key = {fds321098}
}
@article{fds308129,
Author = {Antos, J and Babik, M and Benjamin, D and Cabrera, S and Chan, AW and Chen,
YC and Coca, M and Cooper, B and Farrington, S and Genser, K and Hatakeyama, K and Hou, S and Hsieh, TL and Jayatilaka, B and Jun, SY and Kotwal, AV and Kraan, AC and Lysak, R and Mandrichenko, IV and Murat, P and Robson, A and Savard, P and Siket, M and Stelzer, B and Syu, J and Teng,
PK and Timm, SC and Tomura, T and Vataga, E and Wolbers,
SA},
Title = {Data processing model for the CDF experiment},
Journal = {IEEE Transactions on Nuclear Science},
Volume = {53},
Number = {5},
Pages = {2897-2906},
Publisher = {Institute of Electrical and Electronics Engineers
(IEEE)},
Year = {2006},
Month = {October},
url = {http://dx.doi.org/10.1109/TNS.2006.881908},
Abstract = {The data processing model for the CDF experiment is
described. Data processing reconstructs events from parallel
data streams taken with different combinations of physics
event triggers and further splits the events into datasets
of specialised physics interests. The design of the
processing control system makes strict requirements on
bookkeeping records, which trace the status of data flies
and event contents during processing and storage. The
computing architecture was updated to meet the mass data
flow of the Run II data collection, recently upgraded to a
maximum rate of 40 MByte/sec. The data processing facility
consists of a large cluster of Linux computers with data
movement managed by the CDF data handling system to a
multi-petaByte Enstore tape library. The latest processing
cycle has achieved a stable speed of 35 MByte/sec (3
TByte/day). It can be readily scaled by increasing CPU and
data-handling capacity as required. © 2006
IEEE.},
Doi = {10.1109/TNS.2006.881908},
Key = {fds308129}
}
@article{fds327864,
Author = {Sen, S and Kotwal, A and Chekanov, S and Gray, L and Tran, NV and Yu,
SS},
Title = {Detectors for superboosted τ-leptons at future circular
colliders},
Journal = {Proceedings of Science},
Volume = {Part F128556},
Year = {2016},
Month = {January},
Abstract = {We study the detector performance of τ-lepton
identification variables at very high energy proton
colliders. We study hadronically-decaying τ-leptons with
transverse momentum in the TeV range. Calorimeters are
benchmarked in various configurations in order to understand
the impact of granularity and resolution on boosted
τ-lepton discrimination.},
Key = {fds327864}
}
@article{fds354094,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Bourdarios, CA and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder,
AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Determination of jet calibration and energy resolution in
proton–proton collisions at √s=8TeV using the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {12},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08477-8},
Abstract = {The jet energy scale, jet energy resolution, and their
systematic uncertainties are measured for jets reconstructed
with the ATLAS detector in 2012 using proton–proton data
produced at a centre-of-mass energy of 8 TeV with an
integrated luminosity of 20fb-1. Jets are reconstructed from
clusters of energy depositions in the ATLAS calorimeters
using the anti-kt algorithm. A jet calibration scheme is
applied in multiple steps, each addressing specific effects
including mitigation of contributions from additional
proton–proton collisions, loss of energy in dead material,
calorimeter non-compensation, angular biases and other
global jet effects. The final calibration step uses several
in situ techniques and corrects for residual effects not
captured by the initial calibration. These analyses measure
both the jet energy scale and resolution by exploiting the
transverse momentum balance in γ + jet, Z + jet, dijet,
and multijet events. A statistical combination of these
measurements is performed. In the central detector region,
the derived calibration has a precision better than 1% for
jets with transverse momentum 150GeV<pT< 1500 GeV, and the
relative energy resolution is (8.4 ± 0.6) % for pT=100GeV
and (23 ± 2) % for pT=20GeV. The calibration scheme for
jets with radius parameter R= 1.0 , for which jets receive a
dedicated calibration of the jet mass, is also
discussed.},
Doi = {10.1140/epjc/s10052-020-08477-8},
Key = {fds354094}
}
@article{fds310308,
Author = {ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Determination of spin and parity of the Higgs boson in the
[Formula: see text] decay channel with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {231},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3436-3},
Abstract = {Studies of the spin and parity quantum numbers of the Higgs
boson in the [Formula: see text] final state are presented,
based on proton-proton collision data collected by the ATLAS
detector at the Large Hadron Collider, corresponding to an
integrated luminosity of 20.3 fb[Formula: see text] at a
centre-of-mass energy of [Formula: see text] TeV. The
Standard Model spin-parity [Formula: see text] hypothesis is
compared with alternative hypotheses for both spin and CP.
The case where the observed resonance is a mixture of the
Standard-Model-like Higgs boson and CP-even ([Formula: see
text]) or CP-odd ([Formula: see text]) Higgs boson in
scenarios beyond the Standard Model is also studied. The
data are found to be consistent with the Standard Model
prediction and limits are placed on alternative spin and CP
hypotheses, including CP mixing in different
scenarios.},
Doi = {10.1140/epjc/s10052-015-3436-3},
Key = {fds310308}
}
@article{fds308226,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and del Signore, K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and di Loreto, G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvirai,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feherg, S and Fein,
D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum,
E and Forden, GE},
Title = {Determination of the absolute jet energy scale in the DO
calorimeters},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {424},
Number = {2},
Pages = {352-394},
Publisher = {Elsevier BV},
Year = {1999},
Month = {March},
url = {http://dx.doi.org/10.1016/S0168-9002(98)01368-0},
Abstract = {The DO detector is used to study pp collisions at the 1800
and 630 GeV center-of-mass energies available at the
Fermilab Tevatron. To measure jets, the detector uses a
sampling calorimeter composed of uranium and liquid argon as
the passive and active media, respectively, Understanding
the jet energy calibration is not only crucial for precision
tests of QCD, but also for the measurement of particle
masses and the determination of physics backgrounds
associated with new phenomena. This paper describes the
energy calibration of jets observed with the DO detector at
the two pp center-of-mass energies in the transverse energy
and pseudorapidity range ET>8 GeV and |η|<3.},
Doi = {10.1016/S0168-9002(98)01368-0},
Key = {fds308226}
}
@article{fds308230,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisenko, N and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak,
Y},
Title = {Determination of the mass of the W boson using the D
detector at the Fermilab Tevatron},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {1},
Pages = {120021+1200249},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.58.012002},
Abstract = {A measurement of the mass of the [Formula Presented] boson
is presented which is based on a sample of 5982 [Formula
Presented] decays observed in [Formula Presented] collisions
at [Formula Presented] TeV with the D detector during the
1992–1993 run. From a fit to the transverse mass spectrum,
combined with measurements of the [Formula Presented] boson
mass, the [Formula Presented] boson mass is measured to be
[Formula Presented] Detailed discussions of the
determination of the absolute energy scale, the measured
efficiencies, and all systematic uncertainties are
presented. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevD.58.012002},
Key = {fds308230}
}
@booklet{Abbott98e,
Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
Alves and E. Amidi and N. Amos and E. W. Anderson and R.
Astur and M. M. Baarmand and A. Baden and V. Balamurali and J. Balderston and B},
Title = {Determination of the mass of the W boson using the D0
detector at the Fermilab Tevatron},
Journal = {Physical Review D},
Volume = {5801},
Number = {1},
Year = {1998},
Month = {July},
Key = {Abbott98e}
}
@article{fds358462,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
S},
Title = {Determination of the parton distribution functions of the
proton from ATLAS measurements of differential
W± and Z boson production in association with
jets},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {7},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2021)223},
Abstract = {This article presents a new set of proton parton
distribution functions, ATLASepWZVjet20, produced in an
analysis at next-to-next-to-leading order in QCD. The new
data sets considered are the measurements of W+ and W−
boson and Z boson production in association with jets in pp
collisions at s = 8 TeV performed by the ATLAS experiment at
the LHC with integrated luminosities of 20.2 fb−1 and 19.9
fb−1, respectively. The analysis also considers the ATLAS
measurements of differential W± and Z boson production at s
= 7 TeV with an integrated luminosity of 4.6 fb−1 and
deep-inelastic-scattering data from e±p collisions at the
HERA accelerator. An improved determination of the sea-quark
densities at high Bjorken x is shown, while confirming a
strange-quark density similar in size to the up- and
down-sea-quark densities in the range x ≲ 0.02 found by
previous ATLAS analyses. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP07(2021)223},
Key = {fds358462}
}
@article{fds363730,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
ATH},
Title = {Determination of the parton distribution functions of the
proton using diverse ATLAS data from pp collisions at √s=7
, 8 and 13 TeV},
Journal = {European Physical Journal C},
Volume = {82},
Number = {5},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10217-z},
Abstract = {This paper presents an analysis at next-to-next-to-leading
order in the theory of quantum chromodynamics for the
determination of a new set of proton parton distribution
functions using diverse measurements in pp collisions at
s=7, 8 and 13 TeV, performed by the ATLAS experiment at the
Large Hadron Collider, together with deep inelastic
scattering data from ep collisions at the HERA collider. The
ATLAS data sets considered are differential cross-section
measurements of inclusive W± and Z/ γ∗ boson production,
W± and Z boson production in association with jets, tt¯
production, inclusive jet production and direct photon
production. In the analysis, particular attention is paid to
the correlation of systematic uncertainties within and
between the various ATLAS data sets and to the impact of
model, theoretical and parameterisation uncertainties. The
resulting set of parton distribution functions is called
ATLASpdf21.},
Doi = {10.1140/epjc/s10052-022-10217-z},
Key = {fds363730}
}
@article{fds313614,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
Title = {Determination of the Ratio of b-Quark Fragmentation
Fractions f(s)/f(d) in pp Collisions at √s=7 TeV with
the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {26},
Pages = {262001},
Year = {2015},
Month = {December},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.115.262001},
Abstract = {With an integrated luminosity of 2.47 fb(-1) recorded
by the ATLAS experiment at the LHC, the exclusive decays
B(s)(0)→J/ψϕ and B(d)(0)→J/ψK(*0) of B mesons
produced in pp collisions at √s=7 TeV are used to
determine the ratio of fragmentation fractions f(s)/f(d).
From the observed B(s)(0)→J/ψϕ and B(d)(0)→J/ψK(*0)
yields, the quantity (f(s)/f(d))[B(B(s)(0)→J/ψϕ)/B(B(d)(0)→J/ψK(*0))]
is measured to be 0.199±0.004(stat)±0.008(syst). Using a
recent theory prediction for [B(B(s)(0)→J/ψϕ)/B(B(d)(0)→J/ψK(*0))]
yields (f(s)/f(d))=0.240±0.004(stat)±0.010(syst)±0.017(th).
This result is based on a new approach that provides a
significant improvement of the world average.},
Doi = {10.1103/physrevlett.115.262001},
Key = {fds313614}
}
@article{fds307693,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B and Clement, C and Clifft, RW},
Title = {Determination of the strange-quark density of the proton
from ATLAS measurements of the W→ℓν and Z→ℓℓ
cross sections.},
Journal = {Physical review letters},
Volume = {109},
Number = {1},
Pages = {012001},
Year = {2012},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.109.012001},
Abstract = {A QCD analysis is reported of ATLAS data on inclusive W(±)
and Z boson production in pp collisions at the LHC, jointly
with ep deep-inelastic scattering data from HERA. The ATLAS
data exhibit sensitivity to the light quark sea composition
and magnitude at Bjorken x∼0.01. Specifically, the data
support the hypothesis of a symmetric composition of the
light quark sea at low x. The ratio of the strange-to-down
sea quark distributions is determined to be
1.00(-0.28)(+0.25) at absolute four-momentum transfer
squared Q(2)=1.9 GeV(2) and x=0.023.},
Doi = {10.1103/physrevlett.109.012001},
Key = {fds307693}
}
@article{fds348506,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic,
M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou,
Y},
Title = {Determination of the strong coupling constant α s from
transverse energy-energy correlations in multijet events at
s = 8 TeV using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {12},
Pages = {872},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5442-0},
Abstract = {Measurements of transverse energy-energy correlations and
their associated asymmetries in multi-jet events using the
ATLAS detector at the LHC are presented. The data used
correspond to s = 8 TeV proton-proton collisions with an
integrated luminosity of 20.2 fb - 1 . The results are
presented in bins of the scalar sum of the transverse
momenta of the two leading jets, unfolded to the particle
level and compared to the predictions from Monte Carlo
simulations. A comparison with next-to-leading-order
perturbative QCD is also performed, showing excellent
agreement within the uncertainties. From this comparison,
the value of the strong coupling constant is extracted for
different energy regimes, thus testing the running of α s (
μ ) predicted in QCD up to scales over 1 TeV . A global fit
to the transverse energy-energy correlation distributions
yields α s ( m Z ) = 0.1162 ± 0.0011 (exp.) - 0.0070 +
0.0084 (theo.) , while a global fit to the asymmetry
distributions yields a value of α s ( m Z ) = 0.1196 ±
0.0013 (exp.) - 0.0045 + 0.0075 (theo.) .},
Doi = {10.1140/epjc/s10052-017-5442-0},
Key = {fds348506}
}
@article{fds313610,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Determination of the top-quark pole mass using tt¯tt¯ +
1-jet events collected with the ATLAS experiment in 7 TeV pp
collisions},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {10},
Publisher = {Springer Nature},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2015)121},
Abstract = {Abstract: The normalized differential cross section for
top-quark pair production in association with at least one
jet is studied as a function of the inverse of the invariant
mass of the tt¯(Formula presented.) + 1-jet system. This
distribution can be used for a precise determination of the
top-quark mass since gluon radiation depends on the mass of
the quarks. The experimental analysis is based on
proton-proton collision data collected by the ATLAS detector
at the LHC with a centre-of-mass energy of 7 TeV
corresponding to an integrated luminosity of 4.6 fb−1. The
selected events were identified using the lepton+jets
top-quark-pair decay channel, where lepton refers to either
an electron or a muon. The observed distribution is compared
to a theoretical prediction at next-to-leading-order
accuracy in quantum chromodynamics using the pole-mass
scheme. With this method, the measured value of the
top-quark pole mass, mtpole, is:mtpole=173.7±1.5stat.±1.4syst.−0.5+1.0theoryGeV.(Formula
presented.). This result represents the most precise
measurement of the top-quark pole mass to date.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP10(2015)121},
Key = {fds313610}
}
@article{fds308263,
Author = {Troutman, RR and Kotwal, A},
Title = {Device model for the amorphous-silicon staggered-electrode
thin-film transistor},
Journal = {IEEE Transactions on Electron Devices},
Volume = {36},
Number = {12},
Pages = {2915-2922},
Year = {1989},
url = {http://dx.doi.org/10.1109/16.40955},
Abstract = {A model for the amorphous-silicon (a-Si) staggered-electrode
thin-film transistor (TFT) that incorporates gate-voltage
dependent mobility for channel current and
space-charge-limited current effects for the source and
drain contacts is discussed. This model is in excellent
agreement with TFT data over a wide range of applied
voltages and for various channel lengths. For the devices
measured, the TFT current depends more sensitively on
effective channel mobility than on space-charge-limited
current through the a-Si layer, but the latter is
responsible for current crowding at low drain voltage.
Because of the two-dimensional current flow under the
contacts, their equivalent lumped element model exhibits a
different power law behavior than that for one-dimensional
current flow in an n+-i-n+ structure. It also shows that a
peak in the differential conductance curve at low drain
voltage is a sensitive indicator of current crowding and
implies a superlinear equivalent lumped element in series
with the intrinsic TFT.},
Doi = {10.1109/16.40955},
Key = {fds308263}
}
@article{fds346173,
Author = {Farid, M and Nicholson, S and Kotwal, A and Akali,
A},
Title = {DIEP breast reconstruction following multiple abdominal
liposuction procedures.},
Journal = {Eplasty},
Volume = {14},
Pages = {e47},
Year = {2014},
Month = {January},
Abstract = {<h4>Objective</h4>Previous abdominal wall surgery is viewed
as a contraindication to abdominal free tissue transfer. We
present two patients who underwent multiple abdominal
liposuction procedures, followed by successful free deep
inferior epigastric artery perforator flap. We review the
literature pertaining to reliability of abdominal free flaps
in those with previous abdominal surgery.<h4>Methods</h4>Review
of case notes and radiological investigations of two
patients, and a PubMed search using the terms "DIEP", "deep
inferior epigastric", "TRAM", "transverse rectus abdominis",
"perforator" and "laparotomy", "abdominal wall",
"liposuction", "liposculpture", "fat graft", "pfannenstiel",
with subsequent appraisal of relevant papers by the first
and second authors.<h4>Results</h4>Patient 1 had 3 episodes
of liposuction from the abdomen for fat grafting to a
reconstructed breast. Subsequent revision reconstruction of
the same breast with DIEP flap was preceded by CT
angiography, which demonstrated normal perforator anatomy.
The reconstruction healed well with no ischaemic
complications. Patient 2 had 5 liposuction procedures from
the abdomen to graft fat to a wide local excision defect.
Recurrence of cancer led to mastectomy and immediate
reconstruction with free DIEP flap. Preoperative MR
angiography demonstrated a large perforator right of the
umbilicus, with which the intraoperative findings were
consistent. The patient had an uneventful recovery and good
healing with no fat necrosis or wound dehiscence.<h4>Conclusions</h4>We
demonstrate that DIEP flaps can safely be raised without
perfusion-related complications following multiple
liposuction procedures to the abdomen. The safe interval
between procedures is difficult to quantify, but we
demonstrate successful free flap after 16
months.},
Key = {fds346173}
}
@article{fds308189,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev,
VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett,
JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings,
MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del
Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and di Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A},
Title = {Differential cross section for w boson production as a
function of transverse momentum in p p̄ collisions at √s
= 1.8 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {513},
Number = {3-4},
Pages = {292-300},
Publisher = {Elsevier BV},
Year = {2001},
Month = {August},
url = {http://dx.doi.org/10.1016/S0370-2693(01)00628-1},
Abstract = {We report a measurement of the differential cross section
for W boson production as a function of its transverse
momentum in proton-antiproton collisions at √s = 1.8 TeV.
The data were collected by the DØ experiment at the
Fermilab Tevatron Collider during 1994-1995 and correspond
to an integrated luminosity of 85 pb-1. The results are in
good agreement with quantum chromodynamics over the entire
range of transverse momentum. © 2001 Elsevier Science
B.V.},
Doi = {10.1016/S0370-2693(01)00628-1},
Key = {fds308189}
}
@article{fds355440,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MM and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Differential cross-section measurements for the electroweak
production of dijets in association with a Z boson in
proton–proton collisions at ATLAS},
Journal = {European Physical Journal C},
Volume = {81},
Number = {2},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08734-w},
Abstract = {Differential cross-section measurements are presented for
the electroweak production of two jets in association with a
Z boson. These measurements are sensitive to the
vector-boson fusion production mechanism and provide a
fundamental test of the gauge structure of the Standard
Model. The analysis is performed using proton–proton
collision data collected by ATLAS at s=13TeV and with an
integrated luminosity of 139fb-1. The differential
cross-sections are measured in the Z→ ℓ+ℓ- decay
channel (ℓ= e, μ) as a function of four observables: the
dijet invariant mass, the rapidity interval spanned by the
two jets, the signed azimuthal angle between the two jets,
and the transverse momentum of the dilepton pair. The data
are corrected for the effects of detector inefficiency and
resolution and are sufficiently precise to distinguish
between different state-of-the-art theoretical predictions
calculated using Powheg+Pythia8, Herwig7+Vbfnlo and
Sherpa 2.2. The differential cross-sections are used to
search for anomalous weak-boson self-interactions using a
dimension-six effective field theory. The measurement of the
signed azimuthal angle between the two jets is found to be
particularly sensitive to the interference between the
Standard Model and dimension-six scattering amplitudes and
provides a direct test of charge-conjugation and parity
invariance in the weak-boson self-interactions.},
Doi = {10.1140/epjc/s10052-020-08734-w},
Key = {fds355440}
}
@article{fds308197,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and di Loreto, G and Draper, P and Ducros, Y and Dudko,
LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T},
Title = {Differential production cross section of Z bosons as a
function of transverse momentum at √s = 1.8
TeV},
Journal = {Physical Review Letters},
Volume = {84},
Number = {13},
Pages = {2792-2797},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.2792},
Abstract = {We present a measurement of the transverse momentum
distribution of Z bosons produced in pp collisions at √s =
1.8 TeV from data collected by the D experiment at the
Fermilab Tevatron Collider. We find good agreement between
our results and current resummation calculations, and also
use our data to extract nonperturbative parameters for a
particular version of the resummation formalism. The
resulting values are significantly more precise than
obtained in previous determinations. © 2000 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.84.2792},
Key = {fds308197}
}
@article{fds321137,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {Differential top-antitop cross-section measurements as a
function of observables constructed from final-state
particles using pp collisions at √s = 7 TeV in the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {6},
Pages = {1-56},
Publisher = {Springer Nature},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2015)100},
Abstract = {Abstract: Various differential cross-sections are measured
in top-quark pair (tt) events produced in proton-proton
collisions at a centre-of-mass energy of √s = 7 TeV at the
LHC with the ATLAS detector. These differential
cross-sections are presented in a data set corresponding to
an integrated luminosity of 4.6 fb−1. The differential
cross-sections are presented in terms of kinematic
variables, such as momentum, rapidity and invariant mass, of
a top-quark proxy referred to as the pseudo-top-quark as
well as the pseudo-top-quark pair system. The dependence of
the measurement on theoretical models is minimal. The
measurements are performed on tt events in the lepton+jets
channel, requiring exactly one charged lepton and at least
four jets with at least two of them tagged as originating
from a b-quark. The hadronic and leptonic pseudo-top-quarks
are defined via the leptonic or hadronic decay mode of the W
boson produced by the top-quark decay in events with a
single charged lepton. Differential cross-section
measurements of the pseudo-top-quark variables are compared
with several Monte Carlo models that implement
next-to-leading order or leading-order multi-leg
matrix-element calculations.},
Doi = {10.1007/JHEP06(2015)100},
Key = {fds321137}
}
@article{fds307930,
Author = {Aaltonen, and T, and others},
Title = {Diffractive $W$ and $Z$ production at the Fermilab
Tevatron},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {11},
Pages = {112004},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.82.112004},
Abstract = {We report on a measurement of the fraction of events with a
W or Z boson which are produced diffractively in p̄p
collisions at √s=1.96TeV, using data from 0.6fb⊃-1 of
integrated luminosity collected with the CDFII detector
equipped with a Roman-pot spectrometer that detects the p̄
from p̄+p→p̄+[X+W/Z]. We find that (1.00±0.11)% of Ws
and (0.88±0.22)% of Zs are produced diffractively in a
region of antiproton or proton fractional momentum loss ξ
of 0.03<ξ<0.10 and 4-momentum transferred squared t of
-1<t<0(GeV/c)2, where we account for the events in which the
proton scatters diffractively while the antiproton
dissociates, p̄+p→[X+W/Z]+p, by doubling the measured
proton dissociation fraction. We also report on searches for
W and Z production in double Pomeron exchange,
p+p̄→p+[X+W/Z]+p̄, and on exclusive Z production,
p̄+p→p̄+Z+p. No signal is seen above background for
these processes, and comparisons are made with expectations.
© 2010 The American Physical Society.},
Doi = {10.1103/PhysRevD.82.112004},
Key = {fds307930}
}
@article{fds307800,
Author = {Aaltonen, T and Albrow, M and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F},
Title = {Diffractive dijet production in p̄p collisions at
√s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.032009},
Abstract = {We report on a study of diffractive dijet production in p̄p
collisions at √s=1.96TeV using the CDF II detector at the
Fermilab Tevatron p̄p collider. A data sample from 310pb -1
of integrated luminosity collected by triggering on a high
transverse energy jet, ETjet, in coincidence with a recoil
antiproton detected in a Roman pot spectrometer is used to
measure the ratio of single-diffractive to inclusive-dijet
event rates as a function of xp ̄ of the interacting parton
in the antiproton, the Bjorken-x, xBjp̄, and a Q2(ETjet)2
in the ranges 10 -3<xBjp̄<10 -1 and 102<Q2<104GeV2,
respectively. Results are presented for the region of
p̄-momentum-loss fraction 0.03<ξ p̄<0.09 and a
four-momentum transfer squared t p̄>-4GeV2. The t p̄
dependence is measured as a function of Q2 and xBjp̄ and
compared with that of inclusive single diffraction
dissociation. We find weak xBjp̄ and Q2 dependencies in the
ratio of single diffractive to inclusive event rates, and no
significant Q2 dependence in the diffractive t p̄
distributions. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.032009},
Key = {fds307800}
}
@booklet{Adams97a,
Author = {M. R. Adams and M. Aderholz and S. Aid and P. L. Anthony and D. A. Averill and M. D. Baker and B. R. Baller and A.
Banerjee and H. M. Braun and T. J. Carroll and H. L. Clark and J. M. Conrad and R. Davisson and I. Derado and A. A.
Bhatti and U. Bratzler a},
Title = {Diffractive production of rho(0)(770) mesons in muon-proton
interactions at 470 GeV},
Journal = {Zeitschrift Fur Physik C-particles And Fields},
Volume = {74},
Number = {2},
Pages = {237 -- 261},
Year = {1997},
Month = {April},
Key = {Adams97a}
}
@article{fds308251,
Author = {Adams, MR and Aderholz, M and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dietrich, FS and Dougherty, W and Dreyer, T and Eckardt,
V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kadija, K and Kaufmann, S and Kennedy, RD and Kinney, ER and Kobrak, HGE and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin,
JG and Nickerson, RB and Novak, J and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Röser, A and Ryan, JJ and Salgado, CW and Schellman,
H and Schmitt, M and Schmitz, N and Schüler, KP and Siegert, G and Skuja,
A and Snow, GA and Söldner-Rembold, S and Spentzouris, P and Stopa, P and Swanson, RA and Venkataramania, H and Wilhelm, M and Wilson, R and Wittek, W and Wolbers, SA and Zeller, GP and Zghiche, A and Zhao,
T},
Title = {Diffractive production of ρ0(770) mesons in
muon-proton interactions at 470 GeV},
Journal = {Zeitschrift fur Physik C-Particles and Fields},
Volume = {74},
Number = {2},
Pages = {237-261},
Publisher = {Springer Nature},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1007/s002880050386},
Abstract = {The diffractive production of ρ0(770) mesons in muon-proton
interactions is studied in the kinematic region 0.15 GeV2 <
Q2 < 20 GeV2 and 20 GeV < v < 420 GeV. The data were
obtained in the Fermilab fixed-target experiment E665 with
primary muons of 470 GeV energy. Results are presented on
the Q2, x and v dependence of the cross section, on the
shape of the π+π- mass spectrum, on the slope of the
diffraction peak and on the production and decay angular
distributions of the ρ0(770). The cross section for
diffractive production of ρ0 by virtual photons on protons
depends mainly on Q2. At fixed Q2, no significant dependence
on x or v is observed. The extrapolation to Q2 = 0 yields a
photoproduction cross section of (10.30 ± 0.33) μb. The
slope of the t′ distribution has a value of (7.0 ± 0.2)
GeV-2, with a tendency to decrease as Q2 increases. The
production and decay angular distributions of the ρ0 depend
strongly on Q2 and are consistent with s-channel helicity
conservation. The ratio R = σL/σT deduced from the decay
angular distributions rises strongly with Q2, passing the
value of 1 at Q2 ≈ 2 GeV2. © Springer-Verlag
1997.},
Doi = {10.1007/s002880050386},
Key = {fds308251}
}
@article{fds356577,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
E and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Arduh, FA and Arguin,
JF and Argyropoulos, S and Arling, JH and Armbruster,
AJ},
Title = {Dijet azimuthal correlations and conditional yields in pp
and p+Pb collisions at sNN=5.02TeV with the ATLAS
detector},
Journal = {Physical Review C},
Volume = {100},
Number = {3},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevC.100.034903},
Abstract = {This paper presents a measurement of forward-forward and
forward-central dijet azimuthal angular correlations and
conditional yields in proton-proton (pp) and proton-lead
(p+Pb) collisions as a probe of the nuclear gluon density in
regions where the fraction of the average momentum per
nucleon carried by the parton entering the hard scattering
is low. In these regions, gluon saturation can modify the
rapidly increasing parton distribution function of the
gluon. The analysis utilizes 25pb-1 of pp data and 360μb-1
of p+Pb data, both at sNN=5.02 TeV, collected in 2015 and
2016, respectively, with the ATLAS detector at the Large
Hadron Collider. The measurement is performed in the
center-of-mass frame of the nucleon-nucleon system in the
rapidity range between -4.0 and 4.0 using the two highest
transverse-momentum jets in each event, with the highest
transverse-momentum jet restricted to the forward rapidity
range. No significant broadening of azimuthal angular
correlations is observed for forward-forward or
forward-central dijets in p+Pb compared to pp collisions.
For forward-forward jet pairs in the proton-going direction,
the ratio of conditional yields in p+Pb collisions to those
in pp collisions is suppressed by approximately 20%, with no
significant dependence on the transverse momentum of the
dijet system. No modification of conditional yields is
observed for forward-central dijets.},
Doi = {10.1103/PhysRevC.100.034903},
Key = {fds356577}
}
@article{fds308214,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G},
Title = {Dijet mass spectrum and a search for quark compositeness in
(p)p collisions at sqrt(s) = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {82},
Number = {12},
Pages = {2457-2462},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.2457},
Abstract = {Using the DZero detector at the 1.8 TeV pbarp Fermilab
Tevatron collider, we have measured the inclusive dijet mass
spectrum in the central pseudorapidity region |eta_jet| <
1.0 for dijet masses greater than 200 Gev/c^2. We have also
measured the ratio of spectra sigma(|eta_jet| <
0.5)/sigma(0.5 < |eta_jet| < 1.0). The order alpha_s^3 QCD
predictions are in good agreement with the data and we rule
out models of quark compositeness with a contact interaction
scale < 2.4 TeV at the 95% confidence level. © 1999 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.82.2457},
Key = {fds308214}
}
@article{fds356774,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Dijet production in √s=7 TeV pp collisions with large
rapidity gaps at the ATLAS experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {754},
Pages = {214-234},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2016.01.028},
Abstract = {A 6.8 nb−1 sample of pp collision data collected under
low-luminosity conditions at s=7TeV by the ATLAS detector at
the Large Hadron Collider is used to study diffractive dijet
production. Events containing at least two jets with
pT>20GeV are selected and analysed in terms of variables
which discriminate between diffractive and non-diffractive
processes. Cross sections are measured differentially in
ΔηF, the size of the observable forward region of
pseudorapidity which is devoid of hadronic activity, and in
an estimator, ξ˜ of the fractional momentum loss of the
proton assuming single diffractive dissociation (pp→pX).
Model comparisons indicate a dominant non-diffractive
contribution up to moderately large ΔηF and small ξ˜
with a diffractive contribution which is significant at the
highest ΔηF and the lowest ξ˜. The rapidity-gap survival
probability is estimated from comparisons of the data in
this latter region with predictions based on diffractive
parton distribution functions.},
Doi = {10.1016/j.physletb.2016.01.028},
Key = {fds356774}
}
@article{fds352894,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asai,
K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou,
EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Besson,
N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona,
M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler,
S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
TM and Casado, MP and Casha, AF and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen,
J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chow, YS and Christopher, LD and Chu, MC and Chu, X},
Title = {Dijet Resonance Search with Weak Supervision Using
sqrt[s]=13 TeV pp Collisions in the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {125},
Number = {13},
Pages = {131801},
Year = {2020},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.125.131801},
Abstract = {This Letter describes a search for narrowly resonant new
physics using a machine-learning anomaly detection procedure
that does not rely on signal simulations for developing the
analysis selection. Weakly supervised learning is used to
train classifiers directly on data to enhance potential
signals. The targeted topology is dijet events and the
features used for machine learning are the masses of the two
jets. The resulting analysis is essentially a
three-dimensional search A→BC, for m_{A}∼O(TeV),
m_{B},m_{C}∼O(100 GeV) and B, C are reconstructed as
large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two
jets. The full run 2 sqrt[s]=13 TeV pp collision
dataset of 139 fb^{-1} recorded by the ATLAS detector
at the Large Hadron Collider is used for the search. There
is no significant evidence of a localized excess in the
dijet invariant mass spectrum between 1.8 and 8.2 TeV.
Cross-section limits for narrow-width A, B, and C particles
vary with m_{A}, m_{B}, and m_{C}. For example, when
m_{A}=3 TeV and m_{B}≳200 GeV, a production
cross section between 1 and 5 fb is excluded at
95% confidence level, depending on m_{C}. For certain
masses, these limits are up to 10 times more sensitive than
those obtained by the inclusive dijet search. These results
are complementary to the dedicated searches for the case
that B and C are standard model bosons.},
Doi = {10.1103/physrevlett.125.131801},
Key = {fds352894}
}
@article{fds307962,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar, P and Beecher, D and Behari, S and Bellettini,
G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Copic, K and Cordelli, M and Cortiana, G and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni,
GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest,
R and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper,
S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Koay, SA and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao,
T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Movilla Fernandez and P and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura,
K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert,
B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi,
F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers,
E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber,
I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer,
B},
Title = {Direct bound on the total decay width of the top quark in pp
collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {4},
Pages = {042001},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.102.042001},
Abstract = {We present the first direct experimental bound on the total
decay width of the top quark, Gamma(t), using 955 pb(-1) of
the Tevatron's pp collisions recorded by the Collider
Detector at Fermilab. We identify 253 top-antitop pair
candidate events. The distribution of reconstructed top
quark mass from these events is fitted to templates
representing different values of the top quark width. Using
a confidence interval based on likelihood-ratio ordering, we
extract an upper limit at 95% C.L. of Gamma(t)<13.1 GeV for
an assumed top quark mass of 175 GeV/c(2).},
Doi = {10.1103/physrevlett.102.042001},
Key = {fds307962}
}
@article{fds365671,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
Title = {Direct constraint on the Higgs–charm coupling from a
search for Higgs boson decays into charm quarks with the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {8},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10588-3},
Abstract = {A search for the Higgs boson decaying into a pair of charm
quarks is presented. The analysis uses proton–proton
collisions to target the production of a Higgs boson in
association with a leptonically decaying W or Z boson. The
dataset delivered by the LHC at a centre-of-mass energy of
[InlineEquation not available: see fulltext.] and recorded
by the ATLAS detector corresponds to an integrated
luminosity of 139 fb-1. Flavour-tagging algorithms are used
to identify jets originating from the hadronisation of charm
quarks. The analysis method is validated with the
simultaneous measurement of WW, WZ and ZZ production, with
observed (expected) significances of 2.6 (2.2) standard
deviations above the background-only prediction for the (W/
Z) Z(→ cc¯) process and 3.8 (4.6) standard deviations for
the (W/ Z) W(→ cq) process. The (W/ Z) H(→ cc¯) search
yields an observed (expected) upper limit of 26 (31) times
the predicted Standard Model cross-section times branching
fraction for a Higgs boson with a mass of [InlineEquation
not available: see fulltext.], corresponding to an observed
(expected) constraint on the charm Yukawa coupling modifier
|κc|<8.5(12.4), at the 95% confidence level. A combination
with the ATLAS (W/ Z) H, H→ bb¯ analysis is performed,
allowing the ratio κc/ κb to be constrained to less than
4.5 at the 95% confidence level, smaller than the ratio of
the b- and c-quark masses, and therefore determines the
Higgs-charm coupling to be weaker than the Higgs-bottom
coupling at the 95% confidence level.},
Doi = {10.1140/epjc/s10052-022-10588-3},
Key = {fds365671}
}
@booklet{Abachi97a,
Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard, J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G},
Title = {Direct measurement of the top quark mass},
Journal = {Physical Review Letters},
Volume = {79},
Number = {7},
Pages = {1197-1202},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.1197},
Abstract = {We measure the top quark mass mt t¯t using pairs produced
in the D0 detector by √s = 1.8 TeV p ¯p collisions in a
125pb-1 exposure at the Fermilab Tevatron. We make a two
constraint fit to mt in t¯t → b W+ ¯bW- final states
with one W decaying to q¯q and the other to ev or μ v.
Events are binned in fit mass versus a measure of
probability for events to be signal rather than background.
Likelihood fits to the data yield mt = 17.3 ± 5.6 (stat) ±
6.2(syst) GeV/c2. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.79.1197},
Key = {Abachi97a}
}
@article{fds308240,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Signore, KD and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Loreto, GD and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Geld, TL and Genik, RJ and Genser, K and Gerber, CE and Gibbard, B and Glenn, S and Gobbi, B and Goldschmidt, A and Gómez, B and Gómez, G and Goncharov,
PI and Solís, JLG and Gordon, H and Goss, LT and Gounder, K and Goussiou,
A and Graf, N and Grannis, PD and Green, DR and Greenlee, H and Grim, G and Grinstein, S and Grossman, N and Grudberg, P and Grünendahl, S and Guglielmo, G and Guida, JA and Guida, JM and Gupta, A and Gurzhiev, SN and Gutierrez, P and Gutnikov, YE and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hedin, D and Heinson, AP and Heintz, U and Hernández-Montoya, R and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hsieh, F and Ting, H and Tong, H and Huehn,
T and Ito, AS and James, E and Jaques, J and Jerger, SA and Jesik, R and Jiang, JZY and Joffe-Minor, T and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Jun, SY and Jung, CK and Kahn, S and Kalbfleisch, G and Kang, JS and Karmanov, D and Karmgard, D and Kehoe, R and Kelly, ML and Kim, CL and Kim, SK and Klatchko, A and Klima,
B and Klopfenstein, C and Klyukhin, VI and Kochetkov, VI and Kohli, JM and Koltick, D and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kourlas, J and Kozelov, AV and Kozlovski, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kunori, S and Lami, S and Lander, R and Landry, F and Landsberg, G and Lauer, B and Leflat, A and Li,
H and Li, J and Li-Demarteau, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Liu, YC and Lobkowicz, F and Loken, SC and Lökös, S and Lueking, L and Lyon, AL and Maciel, AKA and Madaras, RJ and Madden, R and Magaña-Mendoza, L and Manankov, V and Mani, S and Mao,
HS and Markeloff, R and Marshall, T and Martin, MI and Mauritz, KM and May,
B and Mayorov, AA and McCarthy, R and McDonald, J and McKibben, T and McKinley, J and McMahon, T and Melanson, HL and Merkin, M and Merritt,
KW and Miettinen, H and Mincer, A and Mishra, CS and Mokhov, N and Mondal,
NK and Montgomery, HE and Mooney, P and Motta, HD and Murphy, C and Nang,
F and Narain, M and Narasimham, VS and Narayanan, A and Neal, HA and Negret, JP and Nemethy, P and Norman, D and Oesch, L and Oguri, V and Oliveira, E and Oltman, E and Oshima, N and Owen, D and Padley, P and Para,
A and Park, YM and Partridge, R and Parua, N and Paterno, M and Pawlik, B and Perkins, J and Peters, M and Piegaia, R and Piekarz, H and Pischalnikov,
Y and Podstavkov, VM and Pope, BG and Prosper, HB and Protopopescu, S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan, S and Ramirez, O and Rasmussen, L and Reucroft, S and Rijssenbeek, M and Rockwell, T and Roco, M and Roe, NA and Rubinov, P and Ruchti, R and Rutherfoord, J and Sánchez-Hernández, A and Santoro, A and Sawyer, L and Schamberger,
RD and Schellman, H and Sculli, J and Shabalina, E and Shaffer, C and Shankar, HC and Shivpuri, RK and Shupe, M and Singh, H and Singh, JB and Sirotenko, V and Smart, W and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sood, PM and Sosebee,
M and Sotnikova, N and Souza, M and Spadafora, AL and Steinbrück, G and Stephens, RW and Stevenson, ML and Stewart, D and Stichelbaut, F and Stoianova, DA and Stoker, D and Strauss, M and Streets, K and Strovink,
M and Sznajder, A and Tamburello, P and Tarazi, J and Tartaglia, M and Thomas, TLT and Thompson, J and Trippe, TG and Tuts, PM and Varelas, N and Varnes, EW and Vititoe, D and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, G and Warchol, J and Watts, G and Wayne, M and Weerts, H and White,
A and White, JT and Wightman, JA and Willis, S and Wimpenny, SJ and Wirjawan, JVD and Womersley, J and Won, E and Wood, DR and Xu, H and Yamada, R and Yamin, P and Yang, J and Yasuda, T and Yepes, P and Yoshikawa, C and Youssef, S and Yu, J and Yu, Y and Zhu, ZH and Zieminska,
D and Zieminski, A and Zverev, EG and Zylberstejn,
A},
Title = {Direct measurement of the top quark mass by the DO
Collaboration},
Journal = {Physical Review D},
Volume = {58},
Number = {5},
Pages = {DUMMY5},
Year = {1998},
Abstract = {We determine the top quark mass mt using tt pairs produced
in the DØ detector by √s=1.8TeV pp collisions in a 125
pb-1 exposure at the Fermilab Tevatron. We make a two
constraint fit to m1 in tt→bW+bW- final states with one W
boson decaying to qq and the other to ev or μv. Likelihood
fits to the data yield mt(l+jets)= 173.3±5.6 (stat) ±5.5
(syst) GeV/c2. When this result is combined with an analysis
of events in which both W bosons decay into leptons, we
obtain mt= 172.1 ±5.2 (stat) ±4.9 (syst) GeV/c2. An
alternate analysis, using three constraint fits to fixed top
quark masses, gives mt(l+ jets) = 176.0 ±7.9 (stat)± 4.8
(syst) GeV/c2, consistent with the above result. Studies of
kinematic distributions of the top quark candidates are also
presented. © 1998 The American Physical
Society.},
Key = {fds308240}
}
@article{fds308239,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and del Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Direct measurement of the top quark mass by the DØ
Collaboration},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {5},
Pages = {520011-520012+5200139},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {September},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.58.052001},
Abstract = {We determine the top quark mass mt using tt̄ pairs produced
in the DØ deteetor by √s = 1.8 TeV pp̄ collisions in a
125 ph-1 exposure at the Fermilab Tevatron. We make a two
constraint fit to mt in tt̄→bW+b̄W- final states with
one W boson decaying to qq̄ and the other to eν or μν.
Likelihood fits to the data yield mt(l+jets) = 173.3±5.6
(stat) ± 5.5 (syst) GeV/c2. When this result is combined
with an analysis of events in which both W bosons decay into
leptons, we obtain mt = 172.1 ± 5.2 (stat) ± 4.9 (syst)
GeV/c2. An alternate analysis, using three constraint fits
to fixed top quark masses, gives mt(l + jets) = 176.0 ± 7.9
(stat) ± 4.8 (syst) GeV/c2, consistent with the above
result. Studies of kinematic distributions of the top quark
candidates are also presented.},
Doi = {10.1103/PhysRevD.58.052001},
Key = {fds308239}
}
@article{fds307566,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Direct measurement of the total decay width of the top
quark.},
Journal = {Physical review letters},
Volume = {111},
Number = {20},
Pages = {202001},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.111.202001},
Abstract = {We present a measurement of the total decay width of the top
quark using events with top-antitop quark pair candidates
reconstructed in the final state with one charged lepton and
four or more hadronic jets. We use the full Tevatron run II
data set of sqrt[s]=1.96 TeV proton-antiproton
collisions recorded by the CDF II detector. The top quark
mass and the mass of the hadronically decaying W boson are
reconstructed for each event and compared with distributions
derived from simulated signal and background samples to
extract the top quark width (Γtop) and the energy scale of
the calorimeter jets with in situ calibration. For a top
quark mass Mtop=172.5 GeV/c2, we find
1.10<Γtop<4.05 GeV at 68% confidence level, which is
in agreement with the standard model expectation of 1.3 GeV
and is the most precise direct measurement of the top quark
width to date.},
Doi = {10.1103/physrevlett.111.202001},
Key = {fds307566}
}
@article{fds307953,
Author = {Aaltonen, T and others},
Title = {Direct Measurement of the W Production Charge Asymmetry in
pp̅ Collisions at sqrt[s] =1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {18},
Pages = {181801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.181801},
Abstract = {We present the first direct measurement of the W production
charge asymmetry as a function of the W boson rapidity yW in
pp̅ collisions at sqrt[s]=1.96 TeV. We use a sample of
W→eν events in data from 1 fb-1 of integrated
luminosity collected using the CDF II detector. In the
region |yW|<3.0, this measurement is capable of
constraining the ratio of up- and down-quark momentum
distributions in the proton more directly than in previous
measurements of the asymmetry that are functions of the
charged-lepton pseudorapidity.},
Doi = {10.1103/physrevlett.102.181801},
Key = {fds307953}
}
@article{fds308176,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev,
VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett,
JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings,
MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del
Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
T and Feher, S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grünendahl, S and Gupta,
A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hildreth, MD and Hirosky,
R and Hobbs, JD and Hoeneisen, B and Huang, Y and Illingworth, R and Ito,
AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Kehoe, R and Kharchilava, A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov,
AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Leflat, A and Leggett, C and Lehner, F and Li, J and Li, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AKA and Madaras, RJ and Malyshev,
VL and Manankov, V and Mao, HS and Marshall, T and Martin, MI and Martin,
RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald,
J and McMahon, T and Melanson, HL and Merkin, M and Merritt, KW and Miao,
C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov, N and Mondal,
NK and Montgomery, HE and Moore, RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Nunnemann, T and O'Neil, D and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Raja, R and Rajagopalan,
S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Santoro, A and Sawyer,
L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder,
A and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van
Kooten, R and Varelas, N and Vertogradov, LS and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, Z-M and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev, EG and Zylberstejn, A and D0
Collaboration},
Title = {Direct search for charged higgs bosons in decays of top
quarks.},
Journal = {Physical review letters},
Volume = {88},
Number = {15},
Pages = {151803},
Year = {2002},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.88.151803},
Abstract = {We present a search for charged Higgs bosons in decays of
pair-produced top quarks in pp collisions at sqrt[s] = 1.8
TeV recorded by the D0 detector at the Fermilab Tevatron
collider. With no evidence for signal, we exclude most
regions of the ( M(H+/-),tan(beta)) parameter space where
the decay t--> H(+)b has a branching fraction >0.36 and
B(H+/--->tau(nu)(tau)) is large.},
Doi = {10.1103/physrevlett.88.151803},
Key = {fds308176}
}
@article{fds308094,
Author = {Abulencia, and A, and others},
Title = {Direct search for Dirac magnetic monopoles in $p\bar{p}$
collisions at $\sqrt{s} = 1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {20},
Pages = {201801},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.201801},
Abstract = {We search for pair-produced Dirac magnetic monopoles in 35.7
pb-1 of proton-antiproton collisions at s**(1/2) = 1.96 TeV
with the Collider Detector at Fermilab (CDF). We find no
monopole candidates corresponding to a 95\% confidence-level
cross-section limit sigma 360 GeV/c2.},
Doi = {10.1103/physrevlett.96.201801},
Key = {fds308094}
}
@article{fds347467,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos,
SPA and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Ferraz,
VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic,
M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and Bylund,
OB and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cai, H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret,
MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini,
M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney,
RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casper, DW and Castelijn, R and Gimenez,
VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Direct top-quark decay width measurement in the t t ¯
lepton+jets channel at s = 8 TeV with the ATLAS
experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {2},
Pages = {129},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5595-5},
Abstract = {This paper presents a direct measurement of the decay width
of the top quark using t t ¯ events in the lepton+jets
final state. The data sample was collected by the ATLAS
detector at the LHC in proton-proton collisions at a
centre-of-mass energy of 8 TeV and corresponds to an
integrated luminosity of 20.2 fb - 1 . The decay width of
the top quark is measured using a template fit to
distributions of kinematic observables associated with the
hadronically and semileptonically decaying top quarks. The
result, Γ t = 1.76 ± 0.33 ( stat. ) - 0.68 + 0.79 ( syst.
) GeV for a top-quark mass of 172.5 GeV, is consistent with
the prediction of the Standard Model.},
Doi = {10.1140/epjc/s10052-018-5595-5},
Key = {fds347467}
}
@article{fds307895,
Author = {Aaltonen, and T, and others},
Title = {Direct Top-Quark Width Measurement at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {23},
Pages = {232003},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.232003},
Abstract = {We present a measurement of the top-quark width in the
lepton+jets decay channel of tt events produced in p p
collisions at Fermilab's Tevatron collider and collected by
the CDF II detector. From a data sample corresponding to 4.3
fb(-1) of integrated luminosity, we identify 756 candidate
events. The top-quark mass and the mass of the hadronically
decaying W boson that comes from the top-quark decay are
reconstructed for each event and compared with templates of
different top-quark widths (Γ(t)) and deviations from
nominal jet energy scale (Δ(JES)) to perform a simultaneous
fit for both parameters, where Δ(JES) is used for the in
situ calibration of the jet energy scale. By applying a
Feldman-Cousins approach, we establish an upper limit at 95%
confidence level (CL) of Γ(t) <7.6 GeV and a two-sided 68%
CL interval of 0.3 GeV <Γ(t) <4.4 GeV for a top-quark
mass of 172.5 GeV/c(2), which are consistent with the
standard model prediction.},
Doi = {10.1103/PhysRevLett.105.232003},
Key = {fds307895}
}
@article{fds362580,
Author = {Kotwal, AV and Hofmann, S},
Title = {Discrete energy spectrum of Hawking radiation from
Schwarzschild surfaces},
Year = {2002},
Month = {April},
Abstract = {We analyze the allowed energy levels of Hawking radiation
from Schwarzschild surfaces in space-times with large extra
dimensions. From the requirement that the wave functions
associated with these particles be single-valued and obey
radial boundary conditions, we derive an upper bound of
their discrete energy spectrum as a function of the number
of large extra dimensions and the mass of the black hole.
Furthermore, we investigate the spacing of the energy
levels.},
Key = {fds362580}
}
@article{fds347525,
Author = {Kotwal, A and Kotwal, J and Prakash, R and Kotwal,
N},
Title = {Does iodine excess lead to hypothyroidism? Evidence from a
case-control study in India.},
Journal = {Archives of medical research},
Volume = {46},
Number = {6},
Pages = {490-494},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1016/j.arcmed.2015.07.005},
Abstract = {<h4>Background</h4>Iodine deficiency disorders have been
known to mankind since antiquity and various researchers
elucidated the role of iodine in its causation. However,
recent evidence shows that the entire control program
ignored multi-causality and association of increased iodine
intake with hypothyroidism. This study was conducted to
assess differences of iodine intake as measured by urinary
iodine excretion (UIE) between cases of hypothyroidism and
healthy controls.<h4>Methods</h4>A case-control study was
conducted with three groups (cases, hospital controls and
community controls) in two cities of India. Patients with
overt hypothyroidism were cases (n = 150) and were
compared with age, sex and socioeconomic status-matched
hospital (n = 154) and community (n = 488) controls.
Thyroid function tests (T3, T4, TSH) were used as diagnostic
and inclusion criteria. TPOAb and UIE estimation were
carried out for all study participants.<h4>Results</h4>Mean
values of TPOAb and UIE were higher in cases as compared to
hospital controls as well as community controls (p <0.05).
With a cut off of 34 IU/mL for TPOAb, more cases had an
anti-TPO level >34 as compared to hospital controls
(p <0.001) as well as community controls (p <0.001); OR,
0.06 (95% CI, 0.03, 0.12) and 0.08 (0.05, 0.12),
respectively. For UIE cut-off of 300 μg/L, more cases than
hospital controls (p = 0.090) and community controls
(p = 0.001) had higher levels; OR, 0.671, (0.422, 1.066)
and 0.509, (0.348, 0.744), respectively.<h4>Conclusion</h4>The
study has clearly shown that cases of hypothyroidism are
associated with excess iodine intake. Cohort studies to
generate further evidence and an eco-social epidemiological
approach have been suggested as the way forward.},
Doi = {10.1016/j.arcmed.2015.07.005},
Key = {fds347525}
}
@article{fds227089,
Author = {A.V. Kotwal and S. Chekanov and M. Low},
Title = {Double Higgs Boson Production in the 4tau Channel from
Resonances in Longitudinal Vector Boson Scattering at a 100
TeV Collider},
Journal = {Phys.Rev. D.},
Volume = {91},
Number = {114018},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.91.114018},
Doi = {10.1103/PhysRevD.91.114018},
Key = {fds227089}
}
@article{fds310283,
Author = {Kotwal, AV and Chekanov, S and Low, M},
Title = {Double Higgs boson production in the 4τ channel from
resonances in longitudinal vector boson scattering at a 100
TeV collider},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.91.114018},
Abstract = {We discuss the sensitivity of a 100 TeV pp collider to heavy
resonances produced in longitudinal vector-boson scattering
and decaying to a pair of Higgs bosons. A Monte Carlo study
has been performed using the H→ττ decay channel for both
Higgs bosons, comparing the kinematics of such a signal to
the irreducible Standard Model backgrounds. The results are
presented in the context of a phenomenological model of a
resonance (η) coupling to Goldstone modes, VLVL→η→HH,
as can arise in composite Higgs models. With a fractional
width of 70% (20%), the 5σ discovery reach is 4.2 (2.9) TeV
in resonance mass for 10ab-1 of integrated luminosity. We
also discuss the dependence of the mass reach on the
collider energy and integrated luminosity.},
Doi = {10.1103/PhysRevD.91.114018},
Key = {fds310283}
}
@article{fds307529,
Author = {Kotwal, AV and Hays, CP},
Title = {Drift chamber alignment using cosmic rays},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {762},
Pages = {85-99},
Publisher = {Elsevier BV},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1016/j.nima.2014.05.050},
Abstract = {The Collider Detector at Fermilab (CDF) is a general-purpose
experimental apparatus with an inner tracking detector for
measuring charged particles, surrounded by a calorimeter for
measurements of electromagnetic and hadronic showers and a
muon detector system. We present a technique for, and
results of, a precise relative alignment of the drift
chamber wires of the CDF tracker. This alignment has been an
important component of the track momentum calibration, which
is the basis for the charged-lepton calibration for the
measurement of the W boson mass at CDF. © 2014 Elsevier
B.V.},
Doi = {10.1016/j.nima.2014.05.050},
Key = {fds307529}
}
@article{fds307646,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach,
AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes,
JB and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey,
DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, JB and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans,
RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
SL and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow,
BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu,
ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca,
D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron,
ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
RN and Clemens, JC},
Title = {Dynamics of isolated-photon plus jet production in pp
collisions at s=7 TeV with the ATLAS detector},
Journal = {Nuclear Physics B},
Volume = {875},
Number = {3},
Pages = {483-535},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.nuclphysb.2013.07.025},
Abstract = {The dynamics of isolated-photon plus jet production in pp
collisions at a centre-of-mass energy of 7 TeV has been
studied with the ATLAS detector at the LHC using an
integrated luminosity of 37 pb-1. Measurements of
isolated-photon plus jet bin-averaged cross sections are
presented as functions of photon transverse energy, jet
transverse momentum and jet rapidity. In addition, the
bin-averaged cross sections as functions of the difference
between the azimuthal angles of the photon and the jet, the
photon-jet invariant mass and the scattering angle in the
photon-jet centre-of-mass frame have been measured.
Next-to-leading-order QCD calculations are compared to the
measurements and provide a good description of the data,
except for the case of the azimuthal opening angle. © 2013
CERN.},
Doi = {10.1016/j.nuclphysb.2013.07.025},
Key = {fds307646}
}
@article{fds347523,
Author = {Kotwal, J and Kotwal, A and Bhalla, S and Singh, PK and Nair,
V},
Title = {Effectiveness of homocysteine lowering vitamins in
prevention of thrombotic tendency at high altitude area: A
randomized field trial.},
Journal = {Thrombosis research},
Volume = {136},
Number = {4},
Pages = {758-762},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1016/j.thromres.2015.08.001},
Abstract = {<h4>Introduction</h4>A higher risk of thrombosis has been
reported on prolonged stay at high altitude (HAA). Lowering
of homocysteine (Hcy) has been found to reduce the risk of
venous thrombosis. A randomized field trial was conducted
with primary question whether Hcy lowering agents have any
effect on the incidence of thrombosis at HAA amongst Indian
soldiers as compared to existing interventions.<h4>Methods</h4>All
units freshly inducted to HAA were randomized into
intervention (Vit B12 1000 microgram/day, B6 3mg/day & folic
acid 5mg/day) and control arms, with a sample size of 12,000
person-years in each arm.<h4>Results</h4>At the end of one
year stay at HAA, Folate and B 12 levels decreased
significantly in control arm. The levels of Hcy, fibrinogen
and plasminogen activator inhibitor (PAI 1) were lower and
nitric oxide higher in intervention arm as compared to
control arm (p<0.05). At the end of 2years, 5 thrombotic
episodes occurred in the intervention arm and 17 in control
arm with RR of 0.29 (95% CI 0.11-0.80), attributable
fraction % (AFe) 70.59%, Population attributable risk
percent 54.55% and Protective Fraction 240%.<h4>Conclusion</h4>Intervention
with B12 and folic acid is effective in reducing Hcy, PAI 1,
fibrinogen levels and increasing NO levels at 1yr as
compared to control arm and reducing the incidence of
thrombosis at 2years of stay at HAA. Thus, vitamin B 12, B6
and folic acid intervention is safe and effective method of
reducing morbidity and mortality caused by HAA induced
coagulopathy.},
Doi = {10.1016/j.thromres.2015.08.001},
Key = {fds347523}
}
@article{fds347540,
Author = {Kotwal, A and Biswas, D and Kakati, B and Thakuria, B and Bhardwaj,
N},
Title = {Efficacy of anti-pseudomonal antibiotics: need to reconsider
the empirical use of cefepime.},
Journal = {The Indian journal of medical research},
Volume = {140},
Number = {4},
Pages = {560-562},
Year = {2014},
Month = {October},
Key = {fds347540}
}
@article{fds346198,
Author = {Londhe, SM and Kumar, P and Mitra, R and Kotwal, A},
Title = {Efficacy of Second Molar to Achieve Anchorage Control in
Maximum Anchorage Cases.},
Journal = {Medical journal, Armed Forces India},
Volume = {66},
Number = {3},
Pages = {220-224},
Year = {2010},
Month = {July},
url = {http://dx.doi.org/10.1016/s0377-1237(10)80041-3},
Abstract = {<h4>Background</h4>The aim of the study was to assess the
efficacy of inclusion of second molar in treatment at the
outset to reinforce anchorage.<h4>Methods</h4>A comparative
study comprising of 30 maximum anchorage cases to quantify
anchorage loss in two situations was undertaken. Group I
consisted of cases in which only first molars were banded
and Group II consisted of cases where both first and second
molars were banded. A total of seven landmarks were marked
and six measurements were recorded on to the pre-treatment
and post-treatment lateral cephalogram.<h4>Result</h4>The
difference in pre-treatment and post-treatment values of all
the variables were statistically significant (p<0.05) except
maxillary central incisor vertical movement (U1 VER),
implying a significant post-treatment change. Thus in both
the treatment approaches U6 and U1 showed a considerable
amount of movement in horizontal and vertical direction and
there was rotation which brought about change in angular
values.<h4>Conclusion</h4>The study has successfully
quantified the anchorage loss and brought out the advantages
of including second molar in treatment at the outset. Not
only the anchorage loss is minimized but inclusion of second
molar also helps to maximize incisor retraction and helps
control angular movement of molar and incisor. Extra time
required for second molar banding is well spent, as the
benefits are overwhelming.},
Doi = {10.1016/s0377-1237(10)80041-3},
Key = {fds346198}
}
@article{fds346219,
Author = {Kotwal, A and Schmidt, CE},
Title = {Electrical stimulation alters protein adsorption and nerve
cell interactions with electrically conducting
biomaterials.},
Journal = {Biomaterials},
Volume = {22},
Number = {10},
Pages = {1055-1064},
Year = {2001},
Month = {May},
url = {http://dx.doi.org/10.1016/s0142-9612(00)00344-6},
Abstract = {Electrical charges have been shown to enhance nerve
regeneration; however, the mechanisms for this effect are
unclear. One hypothesis is that an electrical stimulus
alters the local electrical fields of extracellular matrix
molecules, changing protein adsorption. We have investigated
this hypothesis--that electrical stimulation increases the
adsorption of serum proteins, specifically fibronectin (FN),
to the electrically conducting polymer polypyrrole (PP),
thereby, increasing neurite extension. PP was used because
electrical stimulation of PP has been shown to significantly
enhance neurite outgrowth, and more importantly, PP can be
formed into conduits to guide nerve regeneration in vivo.
Here, we looked at the effects of electrical stimulation on
protein adsorption when an electrical current was applied to
PP (1) during protein adsorption (immediate stimulation) and
(2) several hours after protein adsorption (delayed
stimulation). We found that immediate stimulation of PP
increases FN adsorption from purified FN and
serum-containing solutions. Correspondingly, PC-12 cells
grown on PP films that had been previously adsorbed with FN
during immediate stimulation expressed longer neurites.
However, for delayed stimulation, no significant differences
in adsorption or neurite outgrowth were observed. These
studies suggest that increased FN adsorption with immediate
electrical stimulation may explain enhanced neurite
extension on electrically stimulated PP.},
Doi = {10.1016/s0142-9612(00)00344-6},
Key = {fds346219}
}
@article{fds218204,
Author = {A.V. Kotwal and C. Hays},
Title = {Electromagnetic Shower Properties in a Lead-Scintillator
Sampling Calorimeter},
Journal = {Nuclear Inst. and Methods in Physics Research,
A},
Volume = {729},
Pages = {25-35},
Year = {2013},
Month = {November},
Key = {fds218204}
}
@article{fds307585,
Author = {Kotwal, AV and Hays, C},
Title = {Electromagnetic shower properties in a lead-scintillator
sampling calorimeter},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {729},
Pages = {25-35},
Publisher = {Elsevier BV},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1016/j.nima.2013.05.185},
Abstract = {The Collider Detector at Fermilab (CDF) is a general-purpose
experimental apparatus with an inner tracking detector for
measuring charged particles, surrounded by a calorimeter for
measurements of electromagnetic and hadronic showers. We
describe a geant4 simulation and parameterization of the
response of the CDF central electromagnetic calorimeter
(CEM) to incident electrons and photons. The detector model
consists of a detailed description of the CEM geometry and
material in the direction of the incident particle's
trajectory, and of the passive material between the tracker
and the CEM. We use geant4 to calculate the distributions
of: the energy that leaks from the back of the CEM, the
energy fraction sampled by the scintillators, and the energy
dependence of the response. We parameterize these
distributions to accurately model electron and photon
response and resolution in a custom simulation for the
measurement of the W boson mass. © 2013 Elsevier
B.V.},
Doi = {10.1016/j.nima.2013.05.185},
Key = {fds307585}
}
@article{fds356616,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA},
Title = {Electron and photon energy calibration with the ATLAS
detector using 2015-2016 LHC proton-proton collision
data},
Journal = {Journal of Instrumentation},
Volume = {14},
Number = {3},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1088/1748-0221/14/03/P03017},
Abstract = {This paper presents the electron and photon energy
calibration obtained with the ATLAS detector using about 36
fb-1 of LHC proton-proton collision data recorded at s=13
TeV in 2015 and 2016. The different calibration steps
applied to the data and the optimization of the
reconstruction of electron and photon energies are
discussed. The absolute energy scale is set using a large
sample of Z boson decays into electron-positron pairs. The
systematic uncertainty in the energy scale calibration
varies between 0.03% to 0.2% in most of the detector
acceptance for electrons with transverse momentum close to
45 GeV . For electrons with transverse momentum of 10 GeV
the typical uncertainty is 0.3% to 0.8% and it varies
between 0.25% and 1% for photons with transverse momentum
around 60 GeV . Validations of the energy calibration with
J/ψ → e+e- decays and radiative Z boson decays are also
presented.},
Doi = {10.1088/1748-0221/14/03/P03017},
Key = {fds356616}
}
@article{fds310357,
Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Electron and photon energy calibration with the ATLAS
detector using LHC Run 1 data},
Journal = {European Physical Journal C},
Volume = {74},
Number = {10},
Pages = {1-48},
Publisher = {Springer Nature},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3071-4},
Abstract = {This paper presents the electron and photon energy
calibration achieved with the ATLAS detector using about
25 fb-1 of LHC proton–proton collision data taken at
centre-of-mass energies of (Equation Present) and 8 TeV.
The reconstruction of electron and photon energies is
optimised using multivariate algorithms. The response of the
calorimeter layers is equalised in data and simulation, and
the longitudinal profile of the electromagnetic showers is
exploited to estimate the passive material in front of the
calorimeter and reoptimise the detector simulation. After
all corrections, the Z resonance is used to set the absolute
energy scale. For electrons from Z decays, the achieved
calibration is typically accurate to 0.05 % in most of the
detector acceptance, rising to 0.2 % in regions with large
amounts of passive material. The remaining inaccuracy is
less than 0.2–1 % for electrons with a transverse energy
of 10 GeV, and is on average 0.3 % for photons. The
detector resolution is determined with a relative inaccuracy
of less than 10 % for electrons and photons up to 60 GeV
transverse energy, rising to 40 % for transverse energies
above 500 GeV.},
Doi = {10.1140/epjc/s10052-014-3071-4},
Key = {fds310357}
}
@article{fds356553,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Achary, BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Electron and photon performance measurements with the ATLAS
detector using the 2015-2017 LHC proton-proton collision
data},
Journal = {Journal of Instrumentation},
Volume = {14},
Number = {12},
Year = {2019},
Month = {December},
url = {http://dx.doi.org/10.1088/1748-0221/14/12/P12006},
Abstract = {This paper describes the reconstruction of electrons and
photons with the ATLAS detector, employed for measurements
and searches exploiting the complete LHC Run 2 dataset. An
improved energy clustering algorithm is introduced, and its
implications for the measurement and identification of
prompt electrons and photons are discussed in detail.
Corrections and calibrations that affect performance,
including energy calibration, identification and isolation
efficiencies, and the measurement of the charge of
reconstructed electron candidates are determined using up to
81 fb-1 of proton-proton collision data collected at √s =
13 TeV between 2015 and 2017.},
Doi = {10.1088/1748-0221/14/12/P12006},
Key = {fds356553}
}
@article{fds347495,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten,
K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and da
Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev,
A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
Kuutmann, E and Berger, N and Beringer, J and Berlendis, S and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda,
E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Electron efficiency measurements with the ATLAS detector
using 2012 LHC proton-proton collision data.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {3},
Pages = {195},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4756-2},
Abstract = {This paper describes the algorithms for the reconstruction
and identification of electrons in the central region of the
ATLAS detector at the Large Hadron Collider (LHC). These
algorithms were used for all ATLAS results with electrons in
the final state that are based on the 2012 <i>pp</i>
collision data produced by the LHC at [Formula: see text] =
8 [Formula: see text]. The efficiency of these algorithms,
together with the charge misidentification rate, is measured
in data and evaluated in simulated samples using electrons
from [Formula: see text], [Formula: see text] and [Formula:
see text] decays. For these efficiency measurements, the
full recorded data set, corresponding to an integrated
luminosity of 20.3 fb[Formula: see text], is used. Based on
a new reconstruction algorithm used in 2012, the electron
reconstruction efficiency is 97% for electrons with
[Formula: see text] [Formula: see text] and 99% at
[Formula: see text] [Formula: see text]. Combining this
with the efficiency of additional selection criteria to
reject electrons from background processes or misidentified
hadrons, the efficiency to reconstruct and identify
electrons at the ATLAS experiment varies from 65 to 95%,
depending on the transverse momentum of the electron and
background rejection.},
Doi = {10.1140/epjc/s10052-017-4756-2},
Key = {fds347495}
}
@article{fds307750,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Electron performance measurements with the ATLAS detector
using the 2010 LHC proton-proton collision
data},
Journal = {European Physical Journal C},
Volume = {72},
Number = {3},
Pages = {1-46},
Publisher = {Springer Nature},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-1909-1},
Abstract = {Detailed measurements of the electron performance of the
ATLAS detector at the LHC are reported, using decays of the
Z, W and J/ψ particles. Data collected in 2010 at √s = 7
TeV are used, corresponding to an integrated luminosity of
almost 40 pb-1. The inter-alignment of the inner detector
and the electromagnetic calorimeter, the determination of
the electron energy scale and resolution, and the
performance in terms of response uniformity and linearity
are discussed. The electron identification, reconstruction
and trigger efficiencies, as well as the charge
misidentification probability, are also presented. © 2012
CERN for the benefit of the ATLAS collaboration.},
Doi = {10.1140/epjc/s10052-012-1909-1},
Key = {fds307750}
}
@article{fds310386,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov,
AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji,
W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and De Mendizabal,
JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet,
NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Renstrom, PABD and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Cameron, D and Caminada, LM and Armadans, RC and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cantero, J and Cantrill,
R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland,
W},
Title = {Electron reconstruction and identification efficiency
measurements with the ATLAS detector using the 2011 LHC
proton-proton collision data.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {7},
Pages = {2941},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2941-0},
Abstract = {Many of the interesting physics processes to be measured at
the LHC have a signature involving one or more isolated
electrons. The electron reconstruction and identification
efficiencies of the ATLAS detector at the LHC have been
evaluated using proton-proton collision data collected in
2011 at [Formula: see text] TeV and corresponding to an
integrated luminosity of 4.7 fb[Formula: see text].
Tag-and-probe methods using events with leptonic decays of
[Formula: see text] and [Formula: see text] bosons and
[Formula: see text] mesons are employed to benchmark these
performance parameters. The combination of all measurements
results in identification efficiencies determined with an
accuracy at the few per mil level for electron transverse
energy greater than 30 GeV.},
Doi = {10.1140/epjc/s10052-014-2941-0},
Key = {fds310386}
}
@article{fds349790,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA and Pereira, RA and Arce, ATH and Ardell, RE and Arduh,
FA},
Title = {Electron reconstruction and identification in the ATLAS
experiment using the 2015 and 2016 LHC proton–proton
collision data at √s=13 TeV},
Journal = {European Physical Journal C},
Volume = {79},
Number = {8},
Year = {2019},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7140-6},
Abstract = {Algorithms used for the reconstruction and identification of
electrons in the central region of the ATLAS detector at the
Large Hadron Collider (LHC) are presented in this paper;
these algorithms are used in ATLAS physics analyses that
involve electrons in the final state and which are based on
the 2015 and 2016 proton–proton collision data produced by
the LHC at s = 13 TeV. The performance of the electron
reconstruction, identification, isolation, and charge
identification algorithms is evaluated in data and in
simulated samples using electrons from Z→ ee and J/ ψ→
ee decays. Typical examples of combinations of electron
reconstruction, identification, and isolation operating
points used in ATLAS physics analyses are
shown.},
Doi = {10.1140/epjc/s10052-019-7140-6},
Key = {fds349790}
}
@article{fds362158,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arguin, JF},
Title = {Emulating the impact of additional proton–proton
interactions in the ATLAS simulation by presampling sets of
inelastic Monte Carlo events},
Journal = {Computing and Software for Big Science},
Volume = {6},
Number = {1},
Year = {2022},
Month = {December},
url = {http://dx.doi.org/10.1007/s41781-021-00062-2},
Abstract = {The accurate simulation of additional interactions at the
ATLAS experiment for the analysis of proton–proton
collisions delivered by the Large Hadron Collider presents a
significant challenge to the computing resources. During the
LHC Run 2 (2015–2018), there were up to 70 inelastic
interactions per bunch crossing, which need to be accounted
for in Monte Carlo (MC) production. In this document, a new
method to account for these additional interactions in the
simulation chain is described. Instead of sampling the
inelastic interactions and adding their energy deposits to a
hard-scatter interaction one-by-one, the inelastic
interactions are presampled, independent of the hard
scatter, and stored as combined events. Consequently, for
each hard-scatter interaction, only one such presampled
event needs to be added as part of the simulation chain. For
the Run 2 simulation chain, with an average of 35
interactions per bunch crossing, this new method provides a
substantial reduction in MC production CPU needs of around
20%, while reproducing the properties of the reconstructed
quantities relevant for physics analyses with good
accuracy.},
Doi = {10.1007/s41781-021-00062-2},
Key = {fds362158}
}
@article{fds347524,
Author = {Dewan, E and Biswas, D and Kakati, B and Verma, SK and Kotwal, A and Oberoi, A},
Title = {Epidemiological and mycological characteristics of
candidemia in patients with hematological malignancies
attending a tertiary-care center in India.},
Journal = {Hematology/oncology and stem cell therapy},
Volume = {8},
Number = {3},
Pages = {99-105},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1016/j.hemonc.2015.06.006},
Abstract = {<h4>Background and objectives</h4>We undertook the present
study to ascertain the contributing risk factors and explore
the epidemiological and mycological characteristics of
opportunistic candidemia among patients with hematological
malignancies.<h4>Design and settings</h4>Observational
cross-sectional study in a tertiary care center.<h4>Patients
and methods</h4>Consecutive patients with hematological
malignancies reporting to the collaborating medical and
pediatric units with a febrile episode were recruited and
screened for candidemia by blood culture. Recovered Candida
isolates were speciated and antifungal susceptibility
testing was performed as per Clinical and Laboratory
Standards Institute guideline (CLSI) guidelines M44-A.
Further analysis was done for potential risk factors and
compared between culture positive and negative
patients.<h4>Results</h4>Of 150 patients recruited, the
majority (n=27) were between 51 and 60 years and the male to
female ratio was 1.63:1. Fifteen patients (10%) were culture
positive. The culture positivity was significantly higher in
acute lymphocytic leukemia (ALL) than in non-ALL patients
(p=0.03). There was significant association of candidaemia
with leucopenia, chemotherapeutic drugs, corticosteroids and
presence of indwelling devices. Duration of disease
(p=0.032) and duration of hospitalization (p=0.003) were
significantly prolonged in culture positive patients. C.
tropicalis was the commonest isolate (46.67%), with non-
Candida albicans outnumbering C. albicans in all categories
of hematological malignancies (2.75:1). All isolates of C.
albicans were uniformly sensitive to all the azoles, but
only 50% were sensitive to amphotericin B and none to
nystatin and flucytosine.<h4>Conclusions</h4>This
observational study identifies ALL and chronic lymphocytic
leukemia (CLL) as the forms of hematological malignancy
predominantly associated with candidemia; specifies risk
factors and chemotherapeutic agents predisposing patients
towards its occurrence; reports a preponderance of C.
tropicalis among the causative agents and finds voriconazole
to be the most effective antifungal agent against the
recovered isolates. This information could assist in
tailoring prophylactic and therapeutic antifungal practices
for this infection, according to local epidemiological and
mycological characteristics.},
Doi = {10.1016/j.hemonc.2015.06.006},
Key = {fds347524}
}
@article{fds313598,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Erratum : Measurement of the inclusive jet cross-section in
proton-proton collisions at √s = 7 TeV using 4.5
fb−1 of data with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {9},
Pages = {1-39},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2015)141},
Abstract = {Abstract: It was found that the non-perturbative corrections
calculated using Pythia with the Perugia 2011 tune did not
include the effect of the underlying event. The affected
correction factors were recomputed using the Pythia 6.427
generator. These corrections are applied as baseline to the
NLO pQCD calculations and thus the central values of the
theoretical predictions have changed by a few percent with
the new corrections. This has a minor impact on the
agreement between the data and the theoretical predictions.
Figures 2 and 6 to 13, and all the tables have been updated
with the new values. A few sentences in the discussion in
sections 5.2 and 9 were altered or removed.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP09(2015)141},
Key = {fds313598}
}
@article{fds314798,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Erratum to ATLAS Run 1 searches for direct pair production
of third-generation squarks at the Large Hadron
Collider},
Journal = {European Physical Journal C},
Volume = {76},
Number = {3},
Publisher = {Springer Nature},
Year = {2016},
Month = {March},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3935-x},
Doi = {10.1140/epjc/s10052-016-3935-x},
Key = {fds314798}
}
@article{fds307774,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik,
M},
Title = {Erratum to: "Search for first generation scalar leptoquarks
in pp collisions at s=7TeV with the ATLAS detector" [Phys.
Lett. B 709 (2012) 158]},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {711},
Number = {5},
Pages = {442-455},
Publisher = {Elsevier BV},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2012.03.023},
Doi = {10.1016/j.physletb.2012.03.023},
Key = {fds307774}
}
@article{fds376411,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Erratum to: Higgs boson production cross-section
measurements and their EFT interpretation in the 4 ℓ decay
channel at s = 13 TeV with the ATLAS detector (The European
Physical Journal C, (2020), 80, 10, (957),
10.1140/epjc/s10052-020-8227-9)},
Journal = {European Physical Journal C},
Volume = {81},
Number = {5},
Year = {2021},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09116-6},
Abstract = {When quoting the final cross section result in the text of
the paper (Eur. Phys. J. C 80 (2020) 957), the theory
component of the uncertainty was incorrectly set to 0.04 pb
while the correct value of 0.03 pb was given in Table 8 and
in all other results reported in this paper.},
Doi = {10.1140/epjc/s10052-021-09116-6},
Key = {fds376411}
}
@article{fds355147,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Erratum to: Higgs boson production cross-section
measurements and their EFT interpretation in the 4 ℓ decay
channel at s = 13 TeV with the ATLAS detector (The European
Physical Journal C, (2020), 80, 10, (957),
10.1140/epjc/s10052-020-8227-9)},
Journal = {European Physical Journal C},
Volume = {81},
Number = {1},
Year = {2021},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08644-x},
Abstract = {In the published HTML version of this article, the
affiliations of the authors of the National Research Nuclear
University MEPhI, Moscow, Russia were unfortunately marked
incorrectly.},
Doi = {10.1140/epjc/s10052-020-08644-x},
Key = {fds355147}
}
@article{fds353482,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Erratum to: Measurement of differential cross sections for
single diffractive dissociation in s = 8 TeV pp collisions
using the ATLAS ALFA spectrometer (Journal of High Energy
Physics, (2020), 2020, 2, (42), 10.1007/JHEP02(2020)042)},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2020)182},
Abstract = {The ATLAS collaboration E-mail: atlas.publications@cern.ch
Erratum to: JHEP02(2020)042 ArXiv ePrint: 1911.00453 Figure
5b of the paper [1] contained a misinterpretation in the
comparison between the reported new ATLAS measurement of the
process pp ! Xp and previously published CMS data [2]. The
ATLAS measurement corresponds to cases where either proton
dissociates. In the comparison, the CMS measurement was
assumed to be defined similarly, whereas in fact it includes
the dissociation of only one of the protons. On further
investigation, the comparison between the ATLAS and CMS
measurements is far from straightforward. The double
dissociation (pp → XY ) contribution in the CMS data is
not well constrained and indications from the CMS analysis
suggest it may be significantly larger than was thought
originally. Fuerthermore, the potentially sizeable central
diffraction (pp → pXp) contribution was subtracted in the
ATLAS measurement, but included by CMS. There is also a
small effect associated with the different centre of mass
energies (7 TeV for CMS and 8 TeV for ATLAS). In view of
these complications, the figure has now been withdrawn from
the publication [1].},
Doi = {10.1007/JHEP10(2020)182},
Key = {fds353482}
}
@article{fds361872,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Erratum to: Measurement of hadronic event shapes in high-p
T multijet final states at s = 13 TeV with the
ATLAS detector (Journal of High Energy Physics, (2021),
2021, 1, (188), 10.1007/JHEP01(2021)188)},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {12},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2021)053},
Abstract = {An error in the normalization of the Aplanarity and
D-parameter has been found. Insufficient precision on the
eigenvalue calculation can cause λ3 to be negative,
exclusively in two-jet events, yielding an underestimation
of the inclusive two-jet cross section.},
Doi = {10.1007/JHEP12(2021)053},
Key = {fds361872}
}
@article{fds359999,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Erratum to: Measurement of light-by-light scattering and
search for axion-like particles with 2.2 nb −1
of Pb+Pb data with the ATLAS detector (Journal of High
Energy Physics, (2021), 2021, 3, (243), 10.1007/JHEP03(2021)243)},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)050},
Abstract = {One correction is noted for the paper, which does not affect
the results reported. The right panel of figure 9 is
corrected as it contained the “internal” label, giving
the misleading impression on the credibility of the
figure.},
Doi = {10.1007/JHEP11(2021)050},
Key = {fds359999}
}
@article{fds347447,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho,
J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Erratum to: Measurement of the W boson polarisation
in t t ¯ events from pp collisions at s = 8 TeV in
the lepton + jets channel with ATLAS.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {79},
Number = {1},
Pages = {19},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6520-7},
Abstract = {[This corrects the article DOI: 10.1140/epjc/s10052-017-4819-4.].},
Doi = {10.1140/epjc/s10052-018-6520-7},
Key = {fds347447}
}
@article{fds356746,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Erratum to: Measurement of the charge asymmetry in top-quark
pair production in the lepton-plus-jets final state in pp
collision data at √s = 8 TeV with the ATLAS detector (The
European Physical Journal C, (2016), 76, 2, (87),
10.1140/epjc/s10052-016-3910-6)},
Journal = {European Physical Journal C},
Volume = {77},
Number = {8},
Year = {2017},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5089-x},
Abstract = {In the original paper, Fig. 4 contains the wrong label
preliminary. The label has been fixed, while none of the
results have changed.(Table Presented.).},
Doi = {10.1140/epjc/s10052-017-5089-x},
Key = {fds356746}
}
@article{fds356644,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Erratum to: Measurement of the W-boson mass in pp collisions
at √s=7 TeV with the ATLAS detector (The European Physical
Journal C, (2018), 78, 2, (110), 10.1140/epjc/s10052-017-5475-4)},
Journal = {European Physical Journal C},
Volume = {78},
Number = {11},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6354-3},
Abstract = {It has been found that Figure 30 shows the 68% and 99%
confidence-level contours for the W boson and top quark mass
measurements, instead of the 68% and 95% confidence-level
contours, as stated in the legend.},
Doi = {10.1140/epjc/s10052-018-6354-3},
Key = {fds356644}
}
@article{fds354097,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Erratum to: Measurements of top-quark pair differential and
double-differential cross-sections in the ℓ +jets channel
with pp collisions at s = 13 TeV using the ATLAS detector
[Eur. Phys. J. C 79 (2019) 1028] (The European Physical
Journal C, (2019), 79, 12, (1028), 10.1140/epjc/s10052-019-7525-6)},
Journal = {European Physical Journal C},
Volume = {80},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08541-3},
Abstract = {Corrections for five figures and six tables are noted for
the paper, which do not affect the conclusions
reported.},
Doi = {10.1140/epjc/s10052-020-08541-3},
Key = {fds354097}
}
@article{fds356599,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos, SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella, L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Erratum to: Measurements of W and Z boson production in pp
collisions at s = 5.02 TeV with the ATLAS detector (The
European Physical Journal C, (2019), 79, 2, (128),
10.1140/epjc/s10052-019-6622-x)},
Journal = {European Physical Journal C},
Volume = {79},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6870-9},
Abstract = {It has been found that the theoretical predictions for W and
Z boson cross sections, and for the W boson charge
asymmetry, which are labelled as NNPDF3.1 [1] have in fact
been calculated using the NNPDF3.0 PDF set [2]
instead.},
Doi = {10.1140/epjc/s10052-019-6870-9},
Key = {fds356599}
}
@article{fds350335,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Erratum to: Search for diboson resonances in hadronic final
states in 139 fb −1 of pp collisions at s = 13
TeV with the ATLAS detector (Journal of High Energy Physics,
(2019), 2019, 9, (91), 10.1007/JHEP09(2019)091)},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {6},
Year = {2020},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2020)042},
Abstract = {A mistake was identified for the paper [1] in the treatment
of the radion [2] cross-sections, which resulted in multiple
changes.},
Doi = {10.1007/JHEP06(2020)042},
Key = {fds350335}
}
@article{fds356645,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Erratum to: Search for heavy resonances decaying into a W or
Z boson and a Higgs boson in final states with leptons and
b-jets in 36 fb−1 of √s = 13 TeV pp
collisions with the ATLAS detector (Journal of High Energy
Physics, (2018), 2018, 3, (174), 10.1007/JHEP03(2018)174)},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {11},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2018)051},
Abstract = {One correction is noted for the paper. The exclusion limits
for the gluon-gluon fusion production of an A boson reported
in the conclusions did not correspond to the exclusion plots
shown in figure 6a.},
Doi = {10.1007/JHEP11(2018)051},
Key = {fds356645}
}
@article{fds310261,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Erratum to: Search for new phenomena in final states with an
energetic jet and large missing transverse momentum in pp
collisions at √s=8 TeV with the ATLAS detector (Eur. Phys.
J. C (2015) 75:299, 10.1140/epjc/s10052-015-3517-3)},
Journal = {European Physical Journal C},
Volume = {75},
Number = {9},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3639-7},
Doi = {10.1140/epjc/s10052-015-3639-7},
Key = {fds310261}
}
@article{fds355666,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Erratum to: Search for phenomena beyond the Standard Model
in events with large b-jet multiplicity using the ATLAS
detector at the LHC (The European Physical Journal C,
(2021), 81, 1, (11), 10.1140/epjc/s10052-020-08730-0)},
Journal = {European Physical Journal C},
Volume = {81},
Number = {3},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-08970-8},
Abstract = {In the original HTML version of this article, one
affiliation of the author V. O. Tikhomirov was missing. He
is affiliated to the following two affiliations: P.N.
Lebedev Physical Institute of the Russian Academy of
Sciences, Moscow, Russia National Research Nuclear
University MEPhI, Moscow, Russia The original article has
been corrected.},
Doi = {10.1140/epjc/s10052-021-08970-8},
Key = {fds355666}
}
@article{fds359797,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Erratum to: Search for squarks and gluinos in final states
with one isolated lepton, jets, and missing transverse
momentum at √s = 13 TeV with the ATLAS detector (The
European Physical Journal C, (2021), 81, 7, (600),
10.1140/epjc/s10052-021-09344-w)},
Journal = {European Physical Journal C},
Volume = {81},
Number = {10},
Year = {2021},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09748-8},
Abstract = {In this article the title was incorrectly given as ‘Search
for squarks and gluinos in final states with one isolated
lepton, jets, and missing transverse momentum at √s = 13
with the ATLAS detector’ but should have been ‘Search
for squarks and gluinos in final states with one isolated
lepton, jets, and missing transverse momentum at √s = 13
TeV with the ATLAS detector’. The original article has
been corrected.},
Doi = {10.1140/epjc/s10052-021-09748-8},
Key = {fds359797}
}
@article{fds313600,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Erratum to: Search for supersymmetry in events containing a
same-flavour opposite-sign dilepton pair, jets, and large
missing transverse momentum in √s = 8 TeV pp collisions
with the ATLAS detector (Eur. Phys. J. C, (2015), 75, (318),
10.1140/epjc/s10052-015-3518-2)},
Journal = {European Physical Journal C},
Volume = {75},
Number = {10},
Publisher = {Springer Nature},
Year = {2015},
Month = {October},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3661-9},
Doi = {10.1140/epjc/s10052-015-3661-9},
Key = {fds313600}
}
@article{fds314799,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Erratum to: Study of the spin and parity of the Higgs boson
in diboson decays with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {76},
Number = {3},
Publisher = {Springer Nature},
Year = {2016},
Month = {March},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3934-y},
Doi = {10.1140/epjc/s10052-016-3934-y},
Key = {fds314799}
}
@article{fds307567,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Erratum: Indirect measurement of sin-2θW
(MW) using e+e - pairs in
the Z-boson region with pp̄ collisions at a
center-of-momentum energy of 1.96 TeV (Physical Review D
(2013) 88 (072002))},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.079905},
Doi = {10.1103/PhysRevD.88.079905},
Key = {fds307567}
}
@article{fds352893,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Erratum: Measurement of differential cross sections and W
+ /W − cross-section ratios for W
boson production in association with jets at s = 8 TeV with
the ATLAS detector (Journal of High Energy Physics, (2018),
2018, 5, (77), 10.1007/JHEP05(2018)077)},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2020)048},
Abstract = {Two additions impacting tables 3 and 4 in ref. [1] are
presented in the following. No significant impact is found
for other results or figures in ref. [1].},
Doi = {10.1007/JHEP10(2020)048},
Key = {fds352893}
}
@article{fds307917,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D},
Title = {Erratum: Measurement of particle production and inclusive
differential cross sections in pp̄ collisions at
√s=1.96TeV (Physical Review D - Particles, Fields,
Gravitation and Cosmology)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {82},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.82.119903},
Doi = {10.1103/PhysRevD.82.119903},
Key = {fds307917}
}
@article{fds307968,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
Title = {Erratum: Measurement of the inclusive jet cross section at
the Fermilab Tevatron pp̄ collider using a cone-based jet
algorithm (Physical Review D (2008) 78 (052006))},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.79.119902},
Doi = {10.1103/PhysRevD.79.119902},
Key = {fds307968}
}
@article{fds308076,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
MA},
Title = {Erratum: Measurement of the inclusive jet cross section
using the kT algorithm in pp̄ collisions at s=1.96TeV with
the CDF II detector (Physical Review D - Particles, Fields,
Gravitation and Cosmology (2007) 75, (092006))},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {75},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.75.119901},
Doi = {10.1103/PhysRevD.75.119901},
Key = {fds308076}
}
@article{fds307919,
Author = {Aaltonen, T and Adelman, J and Álvarez Gonzalez, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M},
Title = {Erratum: Measurement of the W+W-
production cross section and search for anomalous WWγ and
WWZ couplings in pp̄ collisions at √s=1.96 TeV (Phys.
Rev. Lett. (2010) 104 (201801))},
Journal = {Physical Review Letters},
Volume = {105},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2010},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.019905},
Doi = {10.1103/PhysRevLett.105.019905},
Key = {fds307919}
}
@article{fds307669,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {Erratum: Novel inclusive search for the Higgs boson in the
four-lepton final state at CDF (Physical Review D (2012) 86
(072012) DOI:10.1103/PhysRevD. 86.072012)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {9},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.86.099902},
Doi = {10.1103/PhysRevD.86.099902},
Key = {fds307669}
}
@article{fds308139,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH},
Title = {Erratum: Search for Bs0 → μ+μ and Bd0 → μ+μ decays
in pp_ collisions with CDF II (Phys. Rev. Lett. (2005) 95
(221805))},
Journal = {Physical Review Letters},
Volume = {95},
Number = {24},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.95.249905},
Doi = {10.1103/PhysRevLett.95.249905},
Key = {fds308139}
}
@article{fds336454,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Erratum: Search for Bs0 →μ+μ- and B0 →μ+μ- decays
with the full CDF Run II data set (Physical Review D (2013)
87 (072003) DOI: 10.1103/PhysRevD.87.072003)},
Journal = {Physical Review D},
Volume = {97},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.97.099901},
Abstract = {V. Krutelyov, of Texas A&M University and the University of
California at Santa Barbara, was erroneously omitted from
the author list.},
Doi = {10.1103/PhysRevD.97.099901},
Key = {fds336454}
}
@article{fds329967,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Sperka, D and Squillacioti, P and Stancari, M and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang, YC},
Title = {Erratum: Search for Bs0→μ+μ- and
B0→μ+μ- decays with CDF II
(Physical Review Letters (2011) 107 (191801))},
Journal = {Physical Review Letters},
Volume = {107},
Number = {23},
Year = {2011},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.239903},
Doi = {10.1103/PhysRevLett.107.239903},
Key = {fds329967}
}
@article{fds307973,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell,
M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A},
Title = {Erratum: Search for high-mass e+e- Resonances in pp̄
collisions at s=1.96TeV (Physical Review Letters (2009) 102
(031801))},
Journal = {Physical Review Letters},
Volume = {102},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevLett.102.059901},
Doi = {10.1103/PhysRevLett.102.059901},
Key = {fds307973}
}
@article{fds355986,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
Title = {Erratum: Search for new non-resonant phenomena in high-mass
dilepton final states with the ATLAS detector (Journal of
High Energy Physics, (2020), 2020, 11, (5),
10.1007/JHEP11(2020)005)},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {4},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2021)142},
Abstract = {The Lagrangian in eq. (2.1) of JHEP11 (2020) 005 has an
erroneous factor of 1/2. The analysis code used for the
results reported in the paper does not have this factor. The
results remain unchanged.},
Doi = {10.1007/JHEP04(2021)142},
Key = {fds355986}
}
@article{fds307555,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Erratum: Search for new phenomena in final states with large
jet multiplicities and missing transverse momentum at √s =
8 TeV proton-proton collisions using the ATLAS experiment
(Journal of High Energy Physics (2013) 10
(130))},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {1},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2014)109},
Doi = {10.1007/JHEP01(2014)109},
Key = {fds307555}
}
@article{fds308030,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
Gonzalez, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
Title = {Erratum: Search for pair production of scalar top quarks
decaying to a τ Lepton and a b quark in pp̄ collisions at
s=1.96TeV (Physical Review Letters (2008) 101
(071802))},
Journal = {Physical Review Letters},
Volume = {101},
Number = {8},
Publisher = {American Physical Society (APS)},
Year = {2008},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.101.089901},
Doi = {10.1103/PhysRevLett.101.089901},
Key = {fds308030}
}
@article{fds310266,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Ålkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Erratum: Search for production of WW/WZ resonances decaying
to a lepton, neutrino and jets in pp collisions at √s = 8
TeV with the ATLAS detector (The European Physical Journal C
(2015) 75 (209) DOI: 10.1140/epjc/s10052-015-3425-6)},
Journal = {European Physical Journal C},
Volume = {75},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3593-4},
Doi = {10.1140/epjc/s10052-015-3593-4},
Key = {fds310266}
}
@article{fds351562,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli,
G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway,
J},
Title = {Erratum: Search for scalar leptoquark pairs decaying to
ννqq in pp collisions at √(s)=1.96 TeV (Physical Review
D (2005) 71 (112001) DOI: 10.1103/PhysRevD.71.112001)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {11},
Year = {2005},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.71.119901},
Abstract = {This paper was published online on 2 June 2005 with a
typographical error in the title. The title should read as
"⋯ √s = 1:96 TeV." The title has been corrected as of 10
June 2005. The title is correct in the printed version of
the journal.},
Doi = {10.1103/PhysRevD.71.119901},
Key = {fds351562}
}
@article{fds356585,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Erratum: Search for supersymmetry in final states with two
same-sign or three leptons and jets using 36
fb−1 of s = 13 TeV pp collision data with the
ATLAS detector (Journal of High Energy Physics, (2017),
2017, 9, (84), 10.1007/JHEP09(2017)084)},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {8},
Year = {2019},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2019)121},
Abstract = {One correction is made to the figure 4e of the
paper.},
Doi = {10.1007/JHEP08(2019)121},
Key = {fds356585}
}
@article{fds307573,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger,
J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz,
D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Evidence for a bottom baryon resonance Λb*0 in CDF
data},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Pages = {071101},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.071101},
Abstract = {Using data from proton-antiproton collisions at √s=1.96
TeV recorded by the CDF II detector at the Fermilab
Tevatron, evidence for the excited resonance state Λb*0 is
presented in its Λb0π -π+ decay followed by the Λb0→Λ
c+π- and Λc+→pK-π+ decays. The analysis is based on a
data sample corresponding to an integrated luminosity of 9.6
fb-1 collected by an online event selection based on
charged-particle tracks displaced from the proton-antiproton
interaction point. The significance of the observed signal
is 3.5σ. The mass of the observed state is found to be
5919.22±0.76 MeV/c2 in agreement with similar findings in
proton-proton collision experiments. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.88.071101},
Key = {fds307573}
}
@article{fds307878,
Author = {Aaltonen, and T, and al, E},
Title = {Evidence for a mass dependent forward-backward asymmetry in
top quark pair production},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {11},
Pages = {112003},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.112003},
Abstract = {We present a new measurement of the inclusive
forward-backward tt̄ production asymmetry and its rapidity
and mass dependence. The measurements are performed with
data corresponding to an integrated luminosity of 5.3fb -1
of pp̄ collisions at √s=1.96TeV, recorded with the CDF-II
Detector at the Fermilab Tevatron. Significant inclusive
asymmetries are observed in both the laboratory frame and
the tt̄ rest frame, and in both cases are found to be
consistent with CP conservation under interchange of t and
t̄. In the tt̄ rest frame, the asymmetry is observed to
increase with the tt̄ rapidity difference, Δy, and with
the invariant mass M tt̄ of the tt̄ system. Fully
corrected parton-level asymmetries are derived in two
regions of each variable, and the asymmetry is found to be
most significant at large Δy and Mtt̄. For
Mtt̄?450GeV/c2, the parton-level asymmetry in the tt̄ rest
frame is Att̄=0.475±0.114 compared to a next-to-leading
order QCD prediction of 0.088±0.013. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.83.112003},
Key = {fds307878}
}
@article{fds307994,
Author = {Aaltonen, T and others},
Title = {Evidence for a Narrow Near-Threshold Structure in the J/ψϕ
Mass Spectrum in B+→J/ψϕK+ Decays},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {24},
Pages = {242002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.242002},
Abstract = {Evidence is reported for a narrow structure near the J/ψϕ
threshold in exclusive B+→J/ψϕK+ decays produced in p̅
p collisions at sqrt[s]=1.96 TeV. A signal of 14
± 5 events, with statistical significance in excess
of 3.8 standard deviations, is observed in a data sample
corresponding to an integrated luminosity of 2.7 fb-1,
collected by the CDF II detector. The mass and natural width
of the structure are measured to be 4143.0 ±
2.9(stat) ± 1.2(syst) MeV/c2 and
11.7-5.0+8.3(stat) ± 3.7(syst) MeV/c2.},
Doi = {10.1103/physrevlett.102.242002},
Key = {fds307994}
}
@article{fds307691,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Alvarez
González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler,
M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto,
G and Bussey, P and Buszello, CP and Buzatu, A and Calamba, A and Calancha,
C and Camacho-Pérez, E and Camarda, S and Campanelli, M and Campbell,
M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
S and Carron, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chakrabarti, S and Chakraborty, D and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chevalier-Théry,
S and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, DK and Cho,
K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Chung, WH and Chung, YS and Cihangir, S and Ciocci, MA and Claes, D and Clark, A and Clarke, C and Clutter, J and Compostella, G and Convery, ME and Conway,
J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox, CA and Cox, DJ and Crescioli, F and Croc, A and Cuevas, J and Culbertson, R and Cutts, D and Dagenhart, D and d'Ascenzo, N and Das, A and Datta, M and Davies, G and de Barbaro, P and de
Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Dell'orso, M and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
SP and d'Errico, M and Desai, S and Deterre, C and Devaughan, K and Devoto,
F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
PF and Dittmann, JR and Dominguez, A and Donati, S and Dong, P and D'Onofrio, M and Dorigo, M and Dorigo, T and Dubey, A and Dudko, LV and Duggan, D and Duperrin, A and Dutt, S and Dyshkant, A and Eads, M and Ebina, K and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Evans, H and Evdokimov, A and Evdokimov, VN and Facini, G and Farrington, S and Feindt, M and Feng, L and Ferbel, T and Fernandez, JP and Ferrazza, C and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Frank, MJ and Franklin, M and Freeman, JC and Fuess, S and Funakoshi, Y and Gallinaro, M and Garcia-Bellido, A and Garcia, JE and García-González, JA and García-Guerra, GA and Garfinkel, AF and Garosi, P and Gavrilov, V and Gay, P and Geng, W and Gerbaudo, D and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Golovanov, G and Gomez-Ceballos, G and Gomez, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Goussiou, A and Grannis, PD and Greder, S and Greenlee,
H and Grenier, G and Grinstein, S and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hagopian, S and Hahn, SR and Haley, J and Halkiadakis, E and Hamaguchi, A and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, D and Hare, M and Harel, A and Harr, RF and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Heck, M and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hewamanage, S and Hildreth,
MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen,
B and Hogan, J and Hohlfeld, M and Hopkins, W and Horn, D and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeans, DT and Jeon, EJ and Jeong,
MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere, A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung, AW and Junk, TR and Juste, A and Kaadze, K and Kajfasz, E and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kasper, PA and Kato, Y and Katsanos, I and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava,
A and Kharzheev, YN and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim,
YK and Kimura, N and Kirby, M and Kiselevich, I and Klimenko, S and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Krop,
D and Kruse, M and Krutelyov, V and Kuhr, T and Kulikov, S and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lammers, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lebrun, P and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Lin,
C-J and Lindgren, M and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lubatti, HJ and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lysak, R and Lys, J and Maciel, AKA and Madar, R and Madrak,
R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G},
Title = {Evidence for a particle produced in association with weak
bosons and decaying to a bottom-antibottom quark pair in
higgs boson searches at the tevatron.},
Journal = {Physical review letters},
Volume = {109},
Number = {7},
Pages = {071804},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.109.071804},
Abstract = {We combine searches by the CDF and D0 Collaborations for the
associated production of a Higgs boson with a W or Z boson
and subsequent decay of the Higgs boson to a
bottom-antibottom quark pair. The data, originating from
Fermilab Tevatron pp collisions at √s = 1.96 TeV,
correspond to integrated luminosities of up to 9.7 fb(-1).
The searches are conducted for a Higgs boson with mass in
the range 100-150 GeV/c(2). We observe an excess of events
in the data compared with the background predictions, which
is most significant in the mass range between 120 and 135
GeV/c(2). The largest local significance is 3.3 standard
deviations, corresponding to a global significance of 3.1
standard deviations. We interpret this as evidence for the
presence of a new particle consistent with the standard
model Higgs boson, which is produced in association with a
weak vector boson and decays to a bottom-antibottom quark
pair.},
Doi = {10.1103/physrevlett.109.071804},
Key = {fds307691}
}
@article{fds351561,
Author = {Acosta, and D, and others},
Title = {Evidence for B/s0 --> Phi Phi decay and measurements of
branching ratio and A(CP) for B+ --> Phi
K+},
Journal = {Phys. Rev. Lett.},
Volume = {95},
Number = {3},
Pages = {031801},
Year = {2005},
url = {http://dx.doi.org/10.1103/physrevlett.95.031801},
Abstract = {http://arxiv.org/abs/hep-ex/0502044},
Doi = {10.1103/physrevlett.95.031801},
Key = {fds351561}
}
@article{fds356536,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Evidence for electroweak production of two jets in
association with a Zγ pair in pp collisions at s=13 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {803},
Year = {2020},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2020.135341},
Abstract = {Evidence for electroweak production of two jets in
association with a Zγ pair in s=13 TeV proton–proton
collisions at the Large Hadron Collider is presented. The
analysis uses data collected by the ATLAS detector in 2015
and 2016 that corresponds to an integrated luminosity of
36.1fb−1. Events that contain a Z boson candidate decaying
leptonically into either e+e− or μ+μ−, a photon, and
two jets are selected. The electroweak component is measured
with observed and expected significances of 4.1 standard
deviations. The fiducial cross-section for electroweak
production is measured to be σZγjj−EW=7.8±2.0fb, in
good agreement with the Standard Model prediction.},
Doi = {10.1016/j.physletb.2020.135341},
Key = {fds356536}
}
@article{fds310352,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baker,
S and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, MF and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch,
A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y},
Title = {Evidence for electroweak production of W±W±jj in pp
collisions at sqrt[s] = 8 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {113},
Number = {14},
Pages = {141803},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.113.141803},
Abstract = {This Letter presents the first study of W(±)W(±)jj,
same-electric-charge diboson production in association with
two jets, using 20.3 fb(-1) of proton-proton collision data
at sqrt[s] = 8 TeV recorded by the ATLAS detector at
the Large Hadron Collider. Events with two reconstructed
same-charge leptons (e(±)e(±), e(±)μ(±), and
μ(±)μ(±)) and two or more jets are analyzed. Production
cross sections are measured in two fiducial regions, with
different sensitivities to the electroweak and strong
production mechanisms. First evidence for W(±)W(±)jj
production and electroweak-only W(±)W(±)jj production is
observed with a significance of 4.5 and 3.6 standard
deviations, respectively. The measured production cross
sections are in agreement with standard model predictions.
Limits at 95% confidence level are set on anomalous quartic
gauge couplings.},
Doi = {10.1103/physrevlett.113.141803},
Key = {fds310352}
}
@article{fds356735,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Evidence for light-by-light scattering in heavy-ion
collisions with the ATLAS detector at the
LHC},
Journal = {Nature Physics},
Volume = {13},
Number = {9},
Pages = {852-858},
Year = {2017},
Month = {September},
url = {http://dx.doi.org/10.1038/nphys4208},
Abstract = {Light-by-light scattering (γγ → γγ) is a
quantum-mechanical process that is forbidden in the
classical theory of electrodynamics. This reaction is
accessible at the Large Hadron Collider thanks to the large
electromagnetic field strengths generated by
ultra-relativistic colliding lead ions. Using 480 μ1 of
lead-lead collision data recorded at a centre-of-mass energy
per nucleon pair of 5.02 TeV by the ATLAS detector, here we
report evidence for light-by-light scattering. A total of 13
candidate events were observed with an expected background
of 2.6 ± 0.7 events. After background subtraction and
analysis corrections, the fiducial cross-section of the
process Pb + Pb (γγ) → Pb(∗) + Pb(∗)γγ,for photon
transverse energy ET > 3GeV, photon absolute pseudorapidity
|η| <2.4, diphoton invariant mass greater than 6GeV,
diphoton transverse momentum lower than 2GeV and diphoton
acoplanarity below 0.01, is measured to be 70 ± 24 (stat.)
±17 (syst.) nb, which is in agreement with the standard
model predictions.},
Doi = {10.1038/nphys4208},
Key = {fds356735}
}
@article{fds307533,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Vázquez, F and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Evidence for s-channel single-top-quark production in events
with one charged lepton and two jets at CDF.},
Journal = {Physical review letters},
Volume = {112},
Number = {23},
Pages = {231804},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.112.231804},
Abstract = {We report evidence for s-channel single-top-quark production
in proton-antiproton collisions at center-of-mass energy
sqrt[s] = 1.96 TeV using a data set that corresponds to an
integrated luminosity of 9.4 fb(-1) collected by the
Collider Detector at Fermilab. We select events consistent
with the s-channel process including two jets and one
leptonically decaying W boson. The observed significance is
3.8 standard deviations with respect to the background-only
prediction. Assuming a top-quark mass of 172.5 GeV/c(2), we
measure the s-channel cross section to be 1.41(-0.42)(+0.44)
pb.},
Doi = {10.1103/physrevlett.112.231804},
Key = {fds307533}
}
@article{fds356769,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Evidence for single top-quark production in the s-channel in
proton–proton collisions at √s=8 TeV with the ATLAS
detector using the Matrix Element Method},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {756},
Pages = {228-246},
Year = {2016},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2016.03.017},
Abstract = {This Letter presents evidence for single top-quark
production in the s-channel using proton–proton collisions
at a centre-of-mass energy of 8 TeV with the ATLAS detector
at the CERN Large Hadron Collider. The analysis is performed
on events containing one isolated electron or muon, large
missing transverse momentum and exactly two b-tagged jets in
the final state. The analysed data set corresponds to an
integrated luminosity of 20.3 fb−1. The signal is
extracted using a maximum-likelihood fit of a discriminant
which is based on the matrix element method and optimized in
order to separate single-top-quark s-channel events from the
main background contributions, which are top-quark pair
production and W boson production in association with
heavy-flavour jets. The measurement leads to an observed
signal significance of 3.2 standard deviations and a
measured cross-section of σs=4.8±0.8(stat.)−1.3+1.6(syst.)
pb, which is consistent with the Standard Model expectation.
The expected significance for the analysis is 3.9 standard
deviations.},
Doi = {10.1016/j.physletb.2016.03.017},
Key = {fds356769}
}
@article{fds307794,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D},
Title = {Evidence for the associated production of a W boson and a
top quark in ATLAS at √s=7TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {716},
Number = {1},
Pages = {142-159},
Publisher = {Elsevier BV},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2012.08.011},
Abstract = {This Letter presents evidence for the associated production
of a W boson and a top quark using 2.05 fb−1 of pp
collision data at s=7TeV accumulated with the ATLAS detector
at the LHC. The analysis is based on the selection of the
dileptonic final states with events featuring two isolated
leptons, electron or muon, with significant transverse
missing momentum and at least one jet. An approach based on
boosted decision trees has been developed to improve the
discrimination of single top-quark Wt events from
background. A template fit to the final classifier
distributions is performed to determine the cross-section.
The result is incompatible with the background-only
hypothesis at the 3.3σ level, the expected sensitivity
assuming the Standard Model production rate being 3.4σ. The
corresponding cross-section is determined and found to be
σWt=16.8±2.9 (stat)±4.9 (syst) pb, in good agreement with
the Standard Model expectation. From this result the CKM
matrix element |Vtb|=1.03−0.19+0.16 is derived assuming
that the Wt production through |Vts| and |Vtd| is
small.},
Doi = {10.1016/j.physletb.2012.08.011},
Key = {fds307794}
}
@article{fds356689,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O},
Title = {Evidence for the associated production of the Higgs boson
and a top quark pair with the ATLAS detector},
Journal = {Physical Review D},
Volume = {97},
Number = {7},
Year = {2018},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.97.072003},
Abstract = {A search for the associated production of the Higgs boson
with a top quark pair (ttH) is reported. The search is
performed in multilepton final states using a data set
corresponding to an integrated luminosity of 36.1 fb-1 of
proton-proton collision data recorded by the ATLAS
experiment at a center-of-mass energy s=13 TeV at the Large
Hadron Collider. Higgs boson decays to WW∗, ττ, and
ZZ∗ are targeted. Seven final states, categorized by the
number and flavor of charged-lepton candidates, are examined
for the presence of the Standard Model Higgs boson with a
mass of 125 GeV and a pair of top quarks. An excess of
events over the expected background from Standard Model
processes is found with an observed significance of 4.1
standard deviations, compared to an expectation of 2.8
standard deviations. The best fit for the ttH production
cross section is σ(ttH)=790-210+230 fb, in agreement with
the Standard Model prediction of 507-50+35 fb. The
combination of this result with other ttH searches from the
ATLAS experiment using the Higgs boson decay modes to bb,
γγ and ZZ∗→4, has an observed significance of 4.2
standard deviations, compared to an expectation of 3.8
standard deviations. This provides evidence for the ttH
production mode.},
Doi = {10.1103/PhysRevD.97.072003},
Key = {fds356689}
}
@article{fds307820,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt,
N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zucchelli, S and CDF Collaboration},
Title = {Evidence for the charmless annihilation decay mode
B(s)(0)→π(+)π(-).},
Journal = {Physical review letters},
Volume = {108},
Number = {21},
Pages = {211803},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.211803},
Abstract = {We search for annihilation decay modes of neutral b mesons
into pairs of charmless charged hadrons with the upgraded
Collider Detector at the Fermilab Tevatron. Using a data
sample corresponding to 6 fb(-1) of integrated luminosity,
we obtain the first evidence for the B(s)(0)→π(+)π(-)
decay, with a significance of 3.7σ, and a measured
branching ratio B(B(s)(0)→π(+)π(-))=(0.57±0.15(stat)±0.10(syst))×10(-6).
A search for the B(0)→K(+)K(-) mode in the same sample
yields a significance of 2.0σ, and a central value estimate
B(B(0)→K(+)K(-))=(0.23±0.10(stat)±0.10(syst))×10(-6).},
Doi = {10.1103/physrevlett.108.211803},
Key = {fds307820}
}
@article{fds308102,
Author = {Acosta, and D, and others},
Title = {Evidence for the exclusive decay B/c+- --> J/psi pi+- and
measurement of the mass of the B/c meson},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {8},
Pages = {082002},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.082002},
Abstract = {We report first evidence for a fully reconstructed decay
mode of the B+/-_c meson in the channel B+/-_c --> J/psi
pi++/-, with J/psi --> mu+ mu-. The analysis is based on an
integrated luminosity of 360 pb-1 in p anti-p collisions at
1.96 TeV center of mass energy collected by the Collider
Detector at Fermilab. We observe 14.6 +/- 4.6 signal events
with a background of 7.1 +/- 0.9 events, and a fit to the
J/psi pi++/- mass spectrum yields a B+/-_c mass of 6285.7
+/- 5.3 (stat) +/- 1.2 (syst) MeV/c2. The probability of a
peak of this magnitude occurring by random fluctuation in
the search region is estimated as 0.012\%.},
Doi = {10.1103/physrevlett.96.082002},
Key = {fds308102}
}
@article{fds356718,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Evidence for the H → bb decay with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {12},
Pages = {1-69},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2017)024},
Abstract = {A search for the decay of the Standard Model Higgs boson
into a bb pair when produced in association with a W or Z
boson is performed with the ATLAS detector. The analysed
data, corresponding to an integrated luminosity of 36.1
fb-1, were collected in proton-proton collisions in Run 2 of
the Large Hadron Collider at a centre-of-mass energy of
13TeV. Final states containing zero, one and two charged
leptons (electrons or muons) are considered, targeting the
decays Z → νν, W → ℓν and Z → ℓℓ. For a Higgs
boson mass of 125 GeV, an excess of events over the expected
background from other Standard Model processes is found with
an observed significance of 3.5 standard deviations,
compared to an expectation of 3.0 standard deviations. This
excess provides evidence for the Higgs boson decay into
b-quarks and for its production in association with a vector
boson. The combination of this result with that of the Run 1
analysis yields a ratio of the measured signal events to the
Standard Model expectation equal to 0.90 ±
0.18(stat.)+0.21-0.19(syst.). Assuming the Standard Model
production cross-section, the results are consistent with
the value of the Yukawa coupling to b-quarks in the Standard
Model.},
Doi = {10.1007/JHEP12(2017)024},
Key = {fds356718}
}
@article{fds375333,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni,
G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann,
E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto,
D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans,
G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey,
PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabrera Urbán and S and Cadamuro,
L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace,
N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty,
D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili,
B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ},
Title = {Evidence for the Higgs Boson Decay to a Z Boson and a Photon
at the LHC.},
Journal = {Physical review letters},
Volume = {132},
Number = {2},
Pages = {021803},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.132.021803},
Abstract = {The first evidence for the Higgs boson decay to a Z boson
and a photon is presented, with a statistical significance
of 3.4 standard deviations. The result is derived from a
combined analysis of the searches performed by the ATLAS and
CMS Collaborations with proton-proton collision datasets
collected at the CERN Large Hadron Collider (LHC) from 2015
to 2018. These correspond to integrated luminosities of
around 140 fb^{-1} for each experiment, at a
center-of-mass energy of 13 TeV. The measured signal yield
is 2.2±0.7 times the standard model prediction, and agrees
with the theoretical expectation within 1.9 standard
deviations.},
Doi = {10.1103/physrevlett.132.021803},
Key = {fds375333}
}
@article{fds310293,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Evidence for the Higgs-boson Yukawa coupling to tau leptons
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {4},
Pages = {1-74},
Publisher = {Springer Nature},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2015)117},
Abstract = {Abstract: Results of a search for H → ττ decays are
presented, based on the full set of proton-proton collision
data recorded by the ATLAS experiment at the LHC during 2011
and 2012. The data correspond to integrated luminosities of
4.5 fb−1 and 20.3 fb−1 at centre-of-mass energies of
√s = 7 TeV and √s = 8 TeV respectively. All combinations
of leptonic (τ→ℓνν¯ with ℓ = e, μ) and hadronic
(τ → hadrons ν) tau decays are considered. An excess of
events over the expected background from other Standard
Model processes is found with an observed (expected)
significance of 4.5 (3.4) standard deviations. This excess
provides evidence for the direct coupling of the recently
discovered Higgs boson to fermions. The measured signal
strength, normalised to the Standard Model expectation, of
μ = 1. 43− 0.37+ 0.43 is consistent with the predicted
Yukawa coupling strength in the Standard Model.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP04(2015)117},
Key = {fds310293}
}
@article{fds356560,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Evidence for the production of three massive vector bosons
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {798},
Year = {2019},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2019.134913},
Abstract = {A search for the production of three massive vector bosons
in proton–proton collisions is performed using data at
s=13 TeV recorded with the ATLAS detector at the Large
Hadron Collider in the years 2015–2017, corresponding to
an integrated luminosity of 79.8 fb−1. Events with two
same-sign leptons ℓ (electrons or muons) and at least two
reconstructed jets are selected to search for
WWW→ℓνℓνqq. Events with three leptons without any
same-flavour opposite-sign lepton pairs are used to search
for WWW→ℓνℓνℓν, while events with three leptons
and at least one same-flavour opposite-sign lepton pair and
one or more reconstructed jets are used to search for
WWZ→ℓνqqℓℓ. Finally, events with four leptons are
analysed to search for WWZ→ℓνℓνℓℓ and
WZZ→qqℓℓℓℓ. Evidence for the joint production of
three massive vector bosons is observed with a significance
of 4.1 standard deviations, where the expectation is 3.1
standard deviations.},
Doi = {10.1016/j.physletb.2019.134913},
Key = {fds356560}
}
@article{fds307583,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and AbdelKhalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and AlconadaVerzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and AlvarezGonzalez, B and Alviggi, MG and Amako, K and AmaralCoutinho, Y and Amelung, C and Ammosov, VV and AmorDosSantos, SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and AperioBella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
M},
Title = {Evidence for the spin-0 nature of the Higgs boson using
ATLAS data},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {726},
Number = {1-3},
Pages = {120-144},
Publisher = {Elsevier BV},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2013.08.026},
Abstract = {Studies of the spin and parity quantum numbers of the Higgs
boson are presented, based on proton-proton collision data
collected by the ATLAS experiment at the LHC. The Standard
Model spin-parity JP=0+ hypothesis is compared with
alternative hypotheses using the Higgs boson decays
H→γγ, H→ZZ*→4ℓ and H→WW*→ℓνℓν, as well
as the combination of these channels. The analysed dataset
corresponds to an integrated luminosity of 20.7 fb-1
collected at a centre-of-mass energy of s=8TeV. For the
H→ZZ*→4ℓ decay mode the dataset corresponding to an
integrated luminosity of 4.6 fb-1 collected at s=7TeV is
included. The data are compatible with the Standard Model
JP=0+ quantum numbers for the Higgs boson, whereas all
alternative hypotheses studied in this Letter, namely some
specific JP=0-, 1+, 1-, 2+ models, are excluded at
confidence levels above 97.8%. This exclusion holds
independently of the assumptions on the coupling strengths
to the Standard Model particles and in the case of the JP=2+
model, of the relative fractions of gluon-fusion and
quark-antiquark production of the spin-2 particle. The data
thus provide evidence for the spin-0 nature of the Higgs
boson, with positive parity being strongly preferred. ©
2013 CERN.},
Doi = {10.1016/j.physletb.2013.08.026},
Key = {fds307583}
}
@article{fds353614,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler,
A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso,
S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Evidence for tt¯ tt¯ production in the multilepton final
state in proton–proton collisions at √s=13 TeV with the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08509-3},
Abstract = {A search is presented for four-top-quark production using an
integrated luminosity of 139 fb- 1 of proton–proton
collision data at a centre-of-mass energy of 13TeV collected
by the ATLAS detector at the LHC. Events are selected if
they contain a same-sign lepton pair or at least three
leptons (electrons or muons). Jet multiplicity, jet flavour
and event kinematics are used to separate signal from the
background through a multivariate discriminant, and
dedicated control regions are used to constrain the dominant
backgrounds. The four-top-quark production cross section is
measured to be 24-6+7 fb. This corresponds to an observed
(expected) significance with respect to the background-only
hypothesis of 4.3 (2.4) standard deviations and provides
evidence for this process.},
Doi = {10.1140/epjc/s10052-020-08509-3},
Key = {fds353614}
}
@article{fds337202,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
J and Thompson, GA and Thomson, E and Tipton, P and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán,
J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka,
J},
Title = {Evidence for tt̄γ production and measurement of
σtt̄γ/σtt̄},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {84},
Number = {3},
Year = {2011},
url = {http://dx.doi.org/10.1103/PhysRevD.84.031104},
Abstract = {Using data corresponding to 6.0fb-1 of pp̄ collisions at
√s=1.96TeV collected by the CDF II detector, we present a
cross section measurement of top-quark pair production with
an additional radiated photon in the central region with 10
GeV or more of transverse energy tt̄γ. The events are
selected by looking for a lepton (ℓ or μ), a photon (γ),
significant transverse momentum imbalance (ET), large total
transverse energy, and three or more jets, with at least one
identified as containing a b quark (b). Using an event
selection optimized for the tt̄γ candidate sample, we also
measure the cross section of tt̄ (σtt̄). We measure the
tt̄γ cross section (σtt̄γ) to be 0.18±0.08pb, and the
ratio of σtt̄γ to σtt̄ to be 0.024±0.009. We observe a
probability of 0.0015 (3.0 standard deviations) of the
background (non-tt̄γ events alone producing 30 events or
more. © 2011 American Physical Society.},
Doi = {10.1103/PhysRevD.84.031104},
Key = {fds337202}
}
@article{fds308221,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and di Loreto, G and Draper, P and Ducros, Y and Dudko,
LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T},
Title = {Evidence of color coherence effects in W + jets events from
pp collisions at √s = 1.8 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {464},
Number = {1-2},
Pages = {145-155},
Publisher = {Elsevier BV},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1016/S0370-2693(99)01015-1},
Abstract = {We report the results of a study of color coherence effects
in pp collisions based on data collected by the DØ detector
during the 1994-1995 run of the Fermilab Tevatron Collider,
at a center of mass energy √s = 1.8 TeV. Initial-to-final
state color interference effects are observed by examining
particle distribution patterns in events with a W boson and
at least one jet. The data are compared to Monte Carlo
simulations with different color coherence implementations
and to an analytic modified-leading-logarithm perturbative
calculation based on the local parton-hadron duality
hypothesis. © 1999 Published by Elsevier Science B.V. All
rights reserved.},
Doi = {10.1016/S0370-2693(99)01015-1},
Key = {fds308221}
}
@article{fds373739,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH},
Title = {Evidence of off-shell Higgs boson production from ZZ
leptonic decay channels and constraints on its total width
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {846},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138223},
Abstract = {This Letter reports on a search for off-shell production of
the Higgs boson using 139 fb−1 of pp collision data at s=
13 TeV collected by the ATLAS detector at the Large Hadron
Collider. The signature is a pair of Z bosons, with
contributions from both the production and subsequent decay
of a virtual Higgs boson and the interference of that
process with other processes. The two observable final
states are ZZ→4ℓ and ZZ→2ℓ2ν with ℓ=e or μ. In
the ZZ→4ℓ final state, a dense Neural Network is used to
enhance analysis sensitivity with respect to matrix
element-based discrimination. The background-only hypothesis
is rejected with an observed (expected) significance of 3.3
(2.2) standard deviations, representing experimental
evidence for off-shell Higgs boson production. Assuming that
no new particles enter the production of the virtual Higgs
boson, its total width can be deduced from the measurement
of its off-shell production cross-section. The measured
total width of the Higgs boson is 4.5−2.5+3.3 MeV, and the
observed (expected) upper limit on the total width is found
to be 10.5 (10.9) MeV at 95% confidence level.},
Doi = {10.1016/j.physletb.2023.138223},
Key = {fds373739}
}
@article{fds310271,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo,
T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell,
SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Evidence of Wγγ Production in pp Collisions at
sqrt[s]=8 TeV and Limits on Anomalous Quartic Gauge
Couplings with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {3},
Pages = {031802},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.115.031802},
Abstract = {This Letter reports evidence of triple gauge boson
production pp→W(ℓν)γγ+X, which is accessible for the
first time with the 8 TeV LHC data set. The fiducial cross
section for this process is measured in a data sample
corresponding to an integrated luminosity of
20.3 fb^{-1}, collected by the ATLAS detector in 2012.
Events are selected using the W boson decay to eν or μν
as well as requiring two isolated photons. The measured
cross section is used to set limits on anomalous quartic
gauge couplings in the high diphoton mass
region.},
Doi = {10.1103/physrevlett.115.031802},
Key = {fds310271}
}
@article{fds307898,
Author = {Aaltonen, and T, and others},
Title = {Exclusion of an Exotic Top Quark with -4/3 Electric Charge
Using Soft Lepton Tagging},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {10},
Pages = {101801},
Publisher = {American Physical Society},
Year = {2010},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.101801},
Abstract = {We present a measurement of the electric charge of the top
quark using pp collisions corresponding to an integrated
luminosity of 2.7 fb(-1) at the CDF II detector. We
reconstruct tt events in the lepton + jets final state. We
use soft lepton taggers to determine the flavor of the b
jets, which we use to reconstruct the top quark's electric
charge and exclude an exotic top quark with -4/3 charge at
95% confidence level. This is the strongest exclusion of the
exotic charge scenario and the first to use soft leptons for
this purpose.},
Doi = {10.1103/PhysRevLett.105.101801},
Key = {fds307898}
}
@article{fds307587,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar,
R},
Title = {Exclusion of exotic top-like quarks with -4/3 electric
charge using jet-charge tagging in single-lepton tt̄ events
at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {3},
Pages = {032003},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.88.032003},
Abstract = {We report on a measurement of the top-quark electric charge
in tt̄ events in which one W boson originating from the
top-quark pair decays into leptons and the other into
hadrons. The event sample was collected by the CDF II
detector in √s=1.96 TeV proton-antiproton collisions and
corresponds to 5.6 fb-1. We find the data to be consistent
with the standard model and exclude the existence of an
exotic quark with -4/3 electric charge and mass of the
conventional top quark at the 99% confidence level. © 2013
American Physical Society.},
Doi = {10.1103/PhysRevD.88.032003},
Key = {fds307587}
}
@booklet{Abbott98p,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G and Fisk, HE and Fisyak, Y and Flattum, E},
Title = {Experimental search for chargino and neutralino production
in supersymmetry models with a light gravitino},
Journal = {Physical Review Letters},
Volume = {80},
Number = {3},
Pages = {442-447},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.442},
Abstract = {We search for inclusive high ETdiphoton events with large
missing transverse energy in pp¯collisions at s=1.8 TeV.
Such events are expected from pair production of charginos
and neutralinos within the framework of the minimal
supersymmetric standard model with a light gravitino. No
excess of events is observed. In that model, and assuming
gaugino mass unification at the GUT scale, we obtain a 95%
C.L. exclusion region in the supersymmetry parameter space
and lower mass bounds of 150 GeV/c2for the lightest chargino
and 77GeV/c2for the lightest neutralino. © 1998 American
Physical Society.},
Doi = {10.1103/PhysRevLett.80.442},
Key = {Abbott98p}
}
@booklet{Adams95a,
Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dhawan, SK and Dietrich, FS and Dougherty, W and Dreyer, T and Eckardt,
V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Hughes, VW and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kobrak, HG and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin,
JG and Nickerson, RB and Novak, J and O'Day, S and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin,
FM},
Title = {Extraction of the Ratio Fn2/Fp2 from Muon-Deuteron and
Muon-Proton Scattering at Small x and Q2.},
Journal = {Physical review letters},
Volume = {75},
Number = {8},
Pages = {1466-1470},
Year = {1995},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.75.1466},
Doi = {10.1103/physrevlett.75.1466},
Key = {Adams95a}
}
@article{fds308200,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk,
HE and Fisyak, Y and Flattum, E},
Title = {Extraction of the width of the W boson from measurements of
[formula presented] and [formula presented] and their
ratio},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {61},
Number = {7},
Pages = {1-22},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.61.072001},
Abstract = {We report on measurements on inclusive cross sections times
branching fractions into electrons for W and Z bosons
produced in (Formula presented) collisions at (Formula
presented) From an integrated luminosity of 84.5 (Formula
presented) recorded in 1994–1995 using the DØ detector at
the Fermilab Tevatron, we determine (Formula presented) and
(Formula presented) From these, we derive (Formula
presented) (Formula presented) and (Formula presented) We
use the latter to set a 95% confidence level upper limit on
the partial decay width of the W boson into nonstandard
model final states, (Formula presented) of 0.213 GeV.
Combining these results with those from the 1992–1993 data
gives (Formula presented) (Formula presented) and a 95% C.L.
upper limit on (Formula presented) of 0.191 GeV. Using a
sample with a luminosity of 505 (Formula presented) taken at
(Formula presented) we measure (Formula presented) © 2000
The American Physical Society.},
Doi = {10.1103/PhysRevD.61.072001},
Key = {fds308200}
}
@article{fds374916,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Fast b-tagging at the high-level trigger of the ATLAS
experiment in LHC Run 3},
Journal = {Journal of Instrumentation},
Volume = {18},
Number = {11},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1088/1748-0221/18/11/P11006},
Abstract = {The ATLAS experiment relies on real-time hadronic jet
reconstruction and b-tagging to record fully hadronic events
containing b-jets. These algorithms require track
reconstruction, which is computationally expensive and could
overwhelm the high-level-trigger farm, even at the reduced
event rate that passes the ATLAS first stage hardware-based
trigger. In LHC Run 3, ATLAS has mitigated these
computational demands by introducing a fast
neural-network-based b-tagger, which acts as a low-precision
filter using input from hadronic jets and tracks. It runs
after a hardware trigger and before the remaining
high-level-trigger reconstruction. This design relies on the
negligible cost of neural-network inference as compared to
track reconstruction, and the cost reduction from limiting
tracking to specific regions of the detector. In the case of
Standard Model HH → bb̄bb̄, a key signature relying on
b-jet triggers, the filter lowers the input rate to the
remaining high-level trigger by a factor of five at the
small cost of reducing the overall signal efficiency by
roughly 2%.},
Doi = {10.1088/1748-0221/18/11/P11006},
Key = {fds374916}
}
@article{fds356591,
Author = {Abada, A and Abbrescia, M and AbdusSalam, SS and Abdyukhanov, I and Fernandez, JA and Abramov, A and Aburaia, M and Acar, AO and Adzic, PR and Agrawal, P and Aguilar-Saavedra, JA and Aguilera-Verdugo, JJ and Aiba, M and Aichinger, I and Aielli, G and Akay, A and Akhundov, A and Aksakal, H and Albacete, JL and Albergo, S and Alekou, A and Aleksa, M and Aleksan, R and Fernandez, RMA and Alexahin, Y and Alía, RG and Alioli,
S and Tehrani, NA and Allanach, BC and Allport, PP and Altınlı, M and Altmannshofer, W and Ambrosio, G and Amorim, D and Amstutz, O and Anderlini, L and Andreazza, A and Andreini, M and Andriatis, A and Andris, C and Andronic, A and Angelucci, M and Antinori, F and Antipov,
SA and Antonelli, M and Antonello, M and Antonioli, P and Antusch, S and Anulli, F and Apolinário, L and Apollinari, G and Apollonio, A and Appelö, D and Appleby, RB and Apyan, A and Arbey, A and Arbuzov, A and Arduini, G and Arı, V and Arias, S and Armesto, N and Arnaldi, R and Arsenyev, SA and Arzeo, M and Asai, S and Aslanides, E and Aßmann, RW and Astapovych, D and Atanasov, M and Atieh, S and Attié, D and Auchmann,
B and Audurier, A and Aull, S and Aumon, S and Aune, S and Avino, F and Avrillaud, G and Aydın, G and Azatov, A and Azuelos, G and Azzi, P and Azzolini, O and Azzurri, P and Bacchetta, N and Bacchiocchi, E and Bachacou, H and Baek, YW and Baglin, V and Bai, Y and Baird, S and Baker,
MJ and Baldwin, MJ and Ball, AH and Ballarino, A and Banerjee, S and Barber, DP and Barducci, D and Barjhoux, P},
Title = {FCC Physics Opportunities: Future Circular Collider
Conceptual Design Report Volume 1},
Journal = {European Physical Journal C},
Volume = {79},
Number = {6},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6904-3},
Abstract = {We review the physics opportunities of the Future Circular
Collider, covering its e+e-, pp, ep and heavy ion
programmes. We describe the measurement capabilities of each
FCC component, addressing the study of electroweak, Higgs
and strong interactions, the top quark and flavour, as well
as phenomena beyond the Standard Model. We highlight the
synergy and complementarity of the different colliders,
which will contribute to a uniquely coherent and ambitious
research programme, providing an unmatchable combination of
precision and sensitivity to new physics.},
Doi = {10.1140/epjc/s10052-019-6904-3},
Key = {fds356591}
}
@article{fds356593,
Author = {Abada, A and Abbrescia, M and AbdusSalam, SS and Abdyukhanov, I and Abelleira Fernandez and J and Abramov, A and Aburaia, M and Acar, AO and Adzic, PR and Agrawal, P and Aguilar-Saavedra, JA and Aguilera-Verdugo, JJ and Aiba, M and Aichinger, I and Aielli, G and Akay, A and Akhundov, A and Aksakal, H and Albacete, JL and Albergo, S and Alekou, A and Aleksa, M and Aleksan, R and Alemany Fernandez and RM and Alexahin, Y and Alía, RG and Alioli, S and Alipour Tehrani and N and Allanach, BC and Allport, PP and Altınlı, M and Altmannshofer, W and Ambrosio, G and Amorim, D and Amstutz, O and Anderlini, L and Andreazza,
A and Andreini, M and Andriatis, A and Andris, C and Andronic, A and Angelucci, M and Antinori, F and Antipov, SA and Antonelli, M and Antonello, M and Antonioli, P and Antusch, S and Anulli, F and Apolinário, L and Apollinari, G and Apollonio, A and Appelö, D and Appleby, RB and Apyan, A and Arbey, A and Arbuzov, A and Arduini, G and Arı, V and Arias, S and Armesto, N and Arnaldi, R and Arsenyev, SA and Arzeo, M and Asai, S and Aslanides, E and Aßmann, RW and Astapovych, D and Atanasov, M and Atieh, S and Attié, D and Auchmann, B and Audurier, A and Aull, S and Aumon, S and Aune, S and Avino, F and Avrillaud, G and Aydın,
G and Azatov, A and Azuelos, G and Azzi, P and Azzolini, O and Azzurri, P and Bacchetta, N and Bacchiocchi, E and Bachacou, H and Baek, YW and Baglin,
V and Bai, Y and Baird, S and Baker, MJ and Baldwin, MJ and Ball, AH and Ballarino, A and Banerjee, S and Barber, DP and Barducci, D and Barjhoux, P},
Title = {FCC-ee: The Lepton Collider: Future Circular Collider
Conceptual Design Report Volume 2},
Journal = {European Physical Journal: Special Topics},
Volume = {228},
Number = {2},
Pages = {261-623},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1140/epjst/e2019-900045-4},
Abstract = {In response to the 2013 Update of the European Strategy for
Particle Physics, the Future Circular Collider (FCC) study
was launched, as an international collaboration hosted by
CERN. This study covers a highest-luminosity high-energy
lepton collider (FCC-ee) and an energy-frontier hadron
collider (FCC-hh), which could, successively, be installed
in the same 100 km tunnel. The scientific capabilities of
the integrated FCC programme would serve the worldwide
community throughout the 21st century. The FCC study also
investigates an LHC energy upgrade, using FCC-hh technology.
This document constitutes the second volume of the FCC
Conceptual Design Report, devoted to the electron-positron
collider FCC-ee. After summarizing the physics discovery
opportunities, it presents the accelerator design,
performance reach, a staged operation scenario, the
underlying technologies, civil engineering, technical
infrastructure, and an implementation plan. FCC-ee can be
built with today’s technology. Most of the FCC-ee
infrastructure could be reused for FCC-hh. Combining
concepts from past and present lepton colliders and adding a
few novel elements, the FCC-ee design promises outstandingly
high luminosity. This will make the FCC-ee a unique
precision instrument to study the heaviest known particles
(Z, W and H bosons and the top quark), offering great direct
and indirect sensitivity to new physics.},
Doi = {10.1140/epjst/e2019-900045-4},
Key = {fds356593}
}
@article{fds356587,
Author = {Abada, A and Abbrescia, M and AbdusSalam, SS and Abdyukhanov, I and Abelleira Fernandez and J and Abramov, A and Aburaia, M and Acar, AO and Adzic, PR and Agrawal, P and Aguilar-Saavedra, JA and Aguilera-Verdugo, JJ and Aiba, M and Aichinger, I and Aielli, G and Akay, A and Akhundov, A and Aksakal, H and Albacete, JL and Albergo, S and Alekou, A and Aleksa, M and Aleksan, R and Alemany Fernandez and RM and Alexahin, Y and Alía, RG and Alioli, S and Alipour Tehrani and N and Allanach, BC and Allport, PP and Altınlı, M and Altmannshofer, W and Ambrosio, G and Amorim, D and Amstutz, O and Anderlini, L and Andreazza,
A and Andreini, M and Andriatis, A and Andris, C and Andronic, A and Angelucci, M and Antinori, F and Antipov, SA and Antonelli, M and Antonello, M and Antonioli, P and Antusch, S and Anulli, F and Apolinário, L and Apollinari, G and Apollonio, A and Appelö, D and Appleby, RB and Apyan, A and Arbey, A and Arbuzov, A and Arduini, G and Arı, V and Arias, S and Armesto, N and Arnaldi, R and Arsenyev, SA and Arzeo, M and Asai, S and Aslanides, E and Aßmann, RW and Astapovych, D and Atanasov, M and Atieh, S and Attié, D and Auchmann, B and Audurier, A and Aull, S and Aumon, S and Aune, S and Avino, F and Avrillaud, G and Aydın,
G and Azatov, A and Azuelos, G and Azzi, P and Azzolini, O and Azzurri, P and Bacchetta, N and Bacchiocchi, E and Bachacou, H and Baek, YW and Baglin,
V and Bai, Y and Baird, S and Baker, MJ and Baldwin, MJ and Ball, AH and Ballarino, A and Banerjee, S and Barber, DP and Barducci, D and Barjhoux, P},
Title = {FCC-hh: The Hadron Collider: Future Circular Collider
Conceptual Design Report Volume 3},
Journal = {European Physical Journal: Special Topics},
Volume = {228},
Number = {4},
Pages = {755-1107},
Year = {2019},
Month = {July},
url = {http://dx.doi.org/10.1140/epjst/e2019-900087-0},
Abstract = {In response to the 2013 Update of the European Strategy for
Particle Physics (EPPSU), the Future Circular Collider (FCC)
study was launched as a world-wide international
collaboration hosted by CERN. The FCC study covered an
energy-frontier hadron collider (FCC-hh), a
highest-luminosity high-energy lepton collider (FCC-ee), the
corresponding 100 km tunnel infrastructure, as well as the
physics opportunities of these two colliders, and a
high-energy LHC, based on FCC-hh technology. This document
constitutes the third volume of the FCC Conceptual Design
Report, devoted to the hadron collider FCC-hh. It summarizes
the FCC-hh physics discovery opportunities, presents the
FCC-hh accelerator design, performance reach, and staged
operation plan, discusses the underlying technologies, the
civil engineering and technical infrastructure, and also
sketches a possible implementation. Combining ingredients
from the Large Hadron Collider (LHC), the high-luminosity
LHC upgrade and adding novel technologies and approaches,
the FCC-hh design aims at significantly extending the energy
frontier to 100 TeV. Its unprecedented centre of-mass
collision energy will make the FCC-hh a unique instrument to
explore physics beyond the Standard Model, offering great
direct sensitivity to new physics and discoveries.},
Doi = {10.1140/epjst/e2019-900087-0},
Key = {fds356587}
}
@article{fds356710,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Femtoscopy with identified charged pions in proton-lead
collisions at √sNN =5.02 TeV with ATLAS},
Journal = {Physical Review C},
Volume = {96},
Number = {6},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevC.96.064908},
Abstract = {Bose-Einstein correlations between identified charged pions
are measured for p+Pb collisions at sNN=5.02TeV using data
recorded by the ATLAS detector at the CERN Large Hadron
Collider corresponding to a total integrated luminosity of
28nb-1. Pions are identified using ionization energy loss
measured in the pixel detector. Two-particle correlation
functions and the extracted source radii are presented as a
function of collision centrality as well as the average
transverse momentum (kT) and rapidity (yππ) of the pair.
Pairs are selected with a rapidity -2<yππ<1 and with an
average transverse momentum 0.1<kT<0.8GeV. The effect of jet
fragmentation on the two-particle correlation function is
studied, and a method using opposite-charge pair data to
constrain its contributions to the measured correlations is
described. The measured source sizes are substantially
larger in more central collisions and are observed to
decrease with increasing pair kT. A correlation of the radii
with the local charged-particle density is demonstrated. The
scaling of the extracted radii with the mean number of
participating nucleons is also used to compare a selection
of initial-geometry models. The cross term Rol is measured
as a function of rapidity, and a nonzero value is observed
with 5.1σ combined significance for -1<yππ<1 in the most
central events.},
Doi = {10.1103/PhysRevC.96.064908},
Key = {fds356710}
}
@article{fds310383,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Fiducial and differential cross sections of Higgs boson
production measured in the four-lepton decay channel in pp
collisions at √s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {738},
Pages = {234-253},
Publisher = {Elsevier BV},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2014.09.054},
Abstract = {Measurements of fiducial and differential cross sections of
Higgs boson production in the H→ZZ*→4ℓ decay channel
are presented. The cross sections are determined within a
fiducial phase space and corrected for detection efficiency
and resolution effects. They are based on 20.3fb-1 of pp
collision data, produced at √s=8 TeV centre-of-mass energy
at the LHC and recorded by the ATLAS detector. The
differential measurements are performed in bins of
transverse momentum and rapidity of the four-lepton system,
the invariant mass of the subleading lepton pair and the
decay angle of the leading lepton pair with respect to the
beam line in the four-lepton rest frame, as well as the
number of jets and the transverse momentum of the leading
jet. The measured cross sections are compared to selected
theoretical calculations of the Standard Model expectations.
No significant deviation from any of the tested predictions
is found.},
Doi = {10.1016/j.physletb.2014.09.054},
Key = {fds310383}
}
@article{fds347510,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis,
S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram,
IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng,
Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin,
V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou,
Y},
Title = {Fiducial, total and differential cross-section measurements
of t-channel single top-quark production in pp
collisions at 8 TeV using data collected by the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {8},
Pages = {531},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5061-9},
Abstract = {Detailed measurements of <i>t</i>-channel single top-quark
production are presented. They use 20.2 fb[Formula: see
text] of data collected by the ATLAS experiment in
proton-proton collisions at a centre-of-mass energy of
8 TeV at the LHC. Total, fiducial and differential
cross-sections are measured for both top-quark and
top-antiquark production. The fiducial cross-section is
measured with a precision of 5.8% (top quark) and 7.8% (top
antiquark), respectively. The total cross-sections are
measured to be [Formula: see text] for top-quark production
and [Formula: see text] for top-antiquark production, in
agreement with the Standard Model prediction. In addition,
the ratio of top-quark to top-antiquark production
cross-sections is determined to be [Formula: see text]. The
differential cross-sections as a function of the transverse
momentum and rapidity of both the top quark and the top
antiquark are measured at both the parton and particle
levels. The transverse momentum and rapidity differential
cross-sections of the accompanying jet from the
<i>t</i>-channel scattering are measured at particle level.
All measurements are compared to various Monte Carlo
predictions as well as to fixed-order QCD calculations where
available.},
Doi = {10.1140/epjc/s10052-017-5061-9},
Key = {fds347510}
}
@article{fds307845,
Author = {Aaltonen, and T, and al, E},
Title = {First Measurement of the Angular Coefficients of {Drell-Yan}
${e}^{+}{e}^{-}$ Pairs in the ${Z}$ Mass Region from
$p\overline{p}$ Collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {24},
Pages = {241801},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.241801},
Abstract = {We report on the first measurement of the angular
distributions of final state electrons in pp¯ → γ*/Z →
e(+)e(-) + X events produced in the Z boson mass region at
√s1.96 TeV. The data sample collected by the CDF II
detector for this result corresponds to 2.1 fb(-1) of
integrated luminosity. The angular distributions are studied
as a function of the transverse momentum of the
electron-positron pair and show good agreement with the
Lam-Tung relation, consistent with a spin-1 description of
the gluon, and demonstrate that, at high values of the
transverse momentum, Z bosons are produced via
quark-antiquark annihilation and quark-gluon Compton
processes.},
Doi = {10.1103/PhysRevLett.106.241801},
Key = {fds307845}
}
@article{fds307906,
Author = {Aaltonen, and T, and others},
Title = {First Measurement of the b-jet Cross Section in Events with
a $W$ Boson in $p \bar{p}$ Collisions at $\sqrt{s} = 1.96$
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {13},
Pages = {131801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.131801},
Abstract = {http://arxiv.org/abs/0909.1505},
Doi = {10.1103/PhysRevLett.104.131801},
Key = {fds307906}
}
@article{fds310269,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {First measurement of the forward-backward asymmetry in
bottom-quark pair production at high mass},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.92.032006},
Abstract = {We measure the particle-level forward-backward production
asymmetry in bb¯ pairs with masses (mbb¯) larger than 150
GeV/c2, using events with hadronic jets and employing jet
charge to distinguish b from b¯. The measurement uses 9.5
fb-1 of pp¯ collisions at a center-of-mass energy of 1.96
TeV recorded by the CDF II detector. The asymmetry as a
function of mbb¯ is consistent with zero, as well as with
the predictions of the standard model. The measurement
disfavors a simple model including an axigluon with a mass
of 200 GeV/c2, whereas a model containing a heavier 345
GeV/c2 axigluon is not excluded.},
Doi = {10.1103/PhysRevD.92.032006},
Key = {fds310269}
}
@article{fds308039,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
Title = {First measurement of the fraction of top-quark pair
production through gluon-gluon fusion},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {78},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2008},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.78.111101},
Abstract = {We present the first measurement of σ(gg→tt̄)/
σ(pp̄→tt̄). We use 0.96fb-1 of s=1.96TeV pp̄ collision
data recorded with the CDF II detector at Fermilab. Using
charged particles with low transverse momentum in tt̄
events, we find σ(gg→ tt̄)/σ(pp̄→tt̄)=0.07±0.14(stat)±0.
07(syst), corresponding to a 95% confidence level upper
limit of 0.33, in agreement with the standard model
next-to-leading-order prediction of 0.15±0.05. © 2008 The
American Physical Society.},
Doi = {10.1103/PhysRevD.78.111101},
Key = {fds308039}
}
@article{fds307901,
Author = {Aaltonen, and T, and others},
Title = {First Measurement of the Ratio $\sigma_{(t\bar{t})} /
\sigma_{(Z/\gamma^*\to ll)}$ and Precise Extraction of the
$t\bar{t}$ Cross Section},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {1},
Pages = {012001},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.012001},
Abstract = {http://arxiv.org/abs/1004.3224},
Doi = {10.1103/PhysRevLett.105.012001},
Key = {fds307901}
}
@article{fds307971,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini,
J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin,
M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, BY and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo,
KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin,
PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen,
AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer,
MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino,
G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt,
MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider,
FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas,
J},
Title = {First measurement of the ratio of branching fractions B(Λb
0→Λc+μ-ν̄μ)/B(Λb 0→Λc+π-)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2009},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.79.032001},
Abstract = {This article presents the first measurement of the ratio of
branching fractions B(Λb0→Λc+μ-ν̄μ)/
B(Λb0→Λc+π-). Measurements in two control samples using
the same technique B(B̄0→D+μ- ν̄μ)/B(B̄0→D+π-)
and B(B̄ 0→D*(2010)+μ-ν̄μ)/ B(B̄0→D*(2010)+π-)
are also reported. The analysis uses data from an integrated
luminosity of approximately 172pb-1 of pp̄ collisions at
s=1.96TeV, collected with the CDF II detector at the
Fermilab Tevatron. The relative branching fractions are
measured to be B(Λb 0→Λc+μ-ν̄μ)B(Λb
0→Λc+π-)=16.6±3.0(stat) ±1.0(syst)+2.6-3.4(PDG)
±0.3(EBR), B(B̄0→D+μ-ν̄μ) B(B̄0→D+π-)=9.9±1.0(stat)
±0.6(syst)±0.4(PDG)± 0.5(EBR), and B(B̄0→D*(
2010)+μ-ν̄μ)B(B̄0→D*( 2010)+π-)=16.5±2.3(stat)
±0.6(syst)±0.5(PDG)± 0.8(EBR). The uncertainties are from
statistics (stat), internal systematics (syst), world
averages of measurements published by the Particle Data
Group or subsidiary measurements in this analysis (PDG), and
unmeasured branching fractions estimated from theory (EBR),
respectively. This article also presents measurements of the
branching fractions of four new Λb 0 semileptonic decays:
Λb0→Λc( 2595)+μ-ν̄μ, Λb0→Λc( 2625)+μ-ν̄μ,
Λb0→Σc( 2455)0π+μ-ν̄μ, and Λb 0→Σc(2455)++π-μ-ν̄μ,
relative to the branching fraction of the Λb0→Λc+μ-
ν̄μ decay. Finally, the transverse-momentum distribution
of Λb0 baryons produced in pp̄ collisions is measured and
found to be significantly different from that of B̄0
mesons, which results in a modification in the production
cross-section ratio σΛb0/σB̄0 with respect to the CDF I
measurement. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.032001},
Key = {fds307971}
}
@article{fds308055,
Author = {Abulencia, and A, and others},
Title = {First Measurement of the Ratio of Central-Electron to
Forward-Electron W Partial Cross Sections in p-pbar
Collisions at sqrt{s} = 1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {25},
Pages = {251801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.251801},
Abstract = {We present a measurement of sigma(p[overline
p]-->W){\AA}~[script B](W-->enu) at sqrt(s)=1.96 TeV, using
electrons identified in the forward region
(1.2-90+95(syst)$\pm$162(lum) pb. Combining this result with
a previous CDF measurement obtained using electrons in the
central region (|eta|},
Doi = {10.1103/physrevlett.98.251801},
Key = {fds308055}
}
@article{fds361222,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and González, BÁ and Amerio,
S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini,
J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin,
M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, BY and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens,
P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao,
T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer,
MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Palencia,
E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks,
B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus,
C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt,
M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber,
I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer,
B},
Title = {First measurement of the tt̄ differential cross section
dσ/dMtt̄ in pp̄ collisions at s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {102},
Number = {22},
Pages = {222003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevLett.102.222003},
Abstract = {We present a measurement of the tt̄ differential cross
section with respect to the tt̄ invariant mass, dσ/dMtt̄,
in pp̄ collisions at s=1.96TeV using an integrated
luminosity of 2.7fb-1 collected by the CDF II experiment.
The tt̄ invariant mass spectrum is sensitive to a variety
of exotic particles decaying into tt̄ pairs. The result is
consistent with the standard model expectation, as modeled
by PYTHIA with CTEQ5L parton distribution functions. © 2009
The American Physical Society.},
Doi = {10.1103/PhysRevLett.102.222003},
Key = {fds361222}
}
@article{fds308052,
Author = {Aaltonen, and T, and others},
Title = {First Measurement of the W Boson Mass in Run II of the
Tevatron},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {15},
Pages = {151801},
Year = {2007},
url = {http://link.aps.org/abstract/PRL/v99/e151801},
Keywords = {W • boson • mass},
Abstract = {We present a measurement of the W-boson mass using 200 pb-1
of data collected in p[overline p] collisions at
sqrt(s)=1.96 TeV by the CDF II detector at run II of the
Fermilab Tevatron. With a sample of 63 964 W-->enu
candidates and 51 128 W-->µnu candidates, we measure MW=80
413$\pm$34stat$\pm$34syst=80 413$\pm$48 MeV/c2. This is the
most precise single measurement of the W-boson mass to
date.},
Doi = {10.1103/physrevlett.99.151801},
Key = {fds308052}
}
@article{fds327184,
Author = {Hays, C and Jayatilaka, B and Kotwal, A and Nodulman, L and Stelzer-Chilton, O and Trischuk, W and Vollrath,
I},
Title = {First Measurement of the W Boson Mass with CDF in Run
II},
Journal = {Journal of Physics: Conference Series},
Volume = {110},
Number = {2},
Pages = {022019-022019},
Publisher = {IOP Publishing},
Year = {2008},
Month = {June},
url = {http://dx.doi.org/10.1088/1742-6596/110/2/022019},
Doi = {10.1088/1742-6596/110/2/022019},
Key = {fds327184}
}
@article{fds308019,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and De
Lorenzo, G and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di
Ruzza, B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt,
J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson,
W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Koay, SA and Kondo,
K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci,
C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak,
R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Mangano, ML and Manousakis, A and Margaroli, F and Marino,
C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan Griso,
S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic,
V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó,
O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A},
Title = {First measurement of W boson production in association with
a single Charm quark in pp collisions at sqrt(s)=1.96
TeV.},
Journal = {Physical review letters},
Volume = {100},
Number = {9},
Pages = {091803},
Year = {2008},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.100.091803},
Abstract = {We present the first measurement of the production cross
section of a W boson with a single charm quark (c) in pp
collisions at sqrt(s)=1.96 TeV, using soft muon tagging of c
jets. In a data sample of approximately 1.8 fb(-1), recorded
with the Collider Detector at Fermilab II detector at the
Fermilab Tevatron, we select events with W+1 or 2 jets. We
use the charge correlation between the W and the muon from
the semileptonic decay of a charm hadron to extract the Wc
signal. We measure sigma Wc(PTc >20 GeV/c,|eta c|<1.5) x
BR(W-->l nu)=9.8+/-3.2 pb, in agreement with theoretical
expectations.},
Doi = {10.1103/physrevlett.100.091803},
Key = {fds308019}
}
@article{fds308135,
Author = {Acosta, and D, and others},
Title = {First measurements of inclusive W and Z cross sections from
Run II of the Tevatron collider},
Journal = {Phys. Rev. Lett.},
Volume = {94},
Number = {9},
Pages = {091803},
Year = {2005},
url = {http://dx.doi.org/10.1103/physrevlett.94.091803},
Abstract = {http://arxiv.org/abs/hep-ex/0406078},
Doi = {10.1103/physrevlett.94.091803},
Key = {fds308135}
}
@article{fds307938,
Author = {Aaltonen, T and others},
Title = {First Observation of B̅ s0→Ds ± K∓ and
Measurement of the Ratio of Branching Fractions B(B̅
s0→Ds ± K∓)/B(B̅ s0→Ds+π-)},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {19},
Pages = {191802},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.191802},
Abstract = {A combined mass and particle identification fit is used to
make the first observation of the decay B̅ s0→Ds ±
K∓ and measure the branching fraction of B̅ s0→Ds
± K∓ relative to B̅ s0→Ds+π-. This analysis
uses 1.2 fb-1 integrated luminosity of pp̅ collisions
at sqrt[s]=1.96 TeV collected with the CDF II detector
at the Fermilab Tevatron collider. We observe a B̅ s0→Ds
± K∓ signal with a statistical significance of
8.1σ and measure B(B̅ s0→Ds ± K∓)/B(B̅
s0→Ds+π-)=0.097 ± 0.018(stat) ±
0.009(syst).},
Doi = {10.1103/physrevlett.103.191802},
Key = {fds307938}
}
@article{fds307944,
Author = {Aaltonen, T and others},
Title = {First Observation of Vector Boson Pairs in a Hadronic Final
State at the Tevatron Collider},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {9},
Pages = {091803},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.091803},
Abstract = {We present the first observation in hadronic collisions of
the electroweak production of vector boson pairs (VV, V=W,
Z) where one boson decays to a dijet final state. The data
correspond to 3.5 fb-1 of integrated luminosity of pp̅
collisions at sqrt[s]=1.96 TeV collected by the CDF II
detector at the Fermilab Tevatron. We observe 1516 ±
239(stat) ± 144(syst) diboson candidate events and
measure a cross section σ(pp̅ →VV+X) of 18.0 ±
2.8(stat) ± 2.4(syst) ± 1.1(lumi) pb, in
agreement with the expectations of the standard
model.},
Doi = {10.1103/physrevlett.103.091803},
Key = {fds307944}
}
@article{fds308027,
Author = {Kotwal, AV and Collaboration, TCDF},
Title = {First Run II Measurement of the W boson Mass},
Journal = {Physical Review D},
Volume = {77},
Number = {112001},
Pages = {48},
Publisher = {American Physical Society (APS)},
Year = {2008},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.77.112001},
Abstract = {We describe a measurement of the W boson mass mW using
200pb-1 of s=1.96TeV pp̄ collision data taken with the CDF
II detector. With a sample of 63964 W→eν candidates and
51128 W→μν candidates, we measure mW=[80.413±0.034(stat)±0.034(sys)=80.413±0.048]GeV/c2.
This is the single most precise mW measurement to date. When
combined with other measured electroweak parameters, this
result further constrains the properties of new unobserved
particles coupling to W and Z bosons. © 2008 The American
Physical Society.},
Doi = {10.1103/PhysRevD.77.112001},
Key = {fds308027}
}
@article{fds307549,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester Iii and WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {First search for exotic Z Boson decays into photons and
neutral pions in hadron collisions.},
Journal = {Physical review letters},
Volume = {112},
Number = {11},
Pages = {111803},
Year = {2014},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.112.111803},
Abstract = {A search for forbidden and exotic Z boson decays in the
diphoton mass spectrum is presented for the first time in
hadron collisions, based on data corresponding to 10.0
fb(-1) of integrated luminosity from proton-antiproton
collisions at √s = 1.96 TeV collected by the CDF
experiment. No evidence of signal is observed, and 95%
credibility level Bayesian upper limits are set on the
branching ratios of decays of the Z boson to a photon and
neutral pion (which is detected as a photon), a pair of
photons, and a pair of neutral pions. The observed branching
ratio limits are 2.01 × 10(-5) for Z → π(0)γ, 1.46 ×
10(-5) for Z → γγ, and 1.52 × 10(-5) for Z →
π(0)π(0). The Z → π(0)γ and Z → γγ limits improve
the most stringent results from other experiments by factors
of 2.6 and 3.6, respectively. The Z → π(0)π(0) branching
ratio limit is the first experimental result on this
decay.},
Doi = {10.1103/physrevlett.112.111803},
Key = {fds307549}
}
@article{fds307843,
Author = {Aaltonen, and T, and al, E},
Title = {First Search for Multijet Resonances in $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
$p\overline{p}$ Collisions},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {4},
Pages = {042001},
Publisher = {American Physical Society},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.042001},
Abstract = {We present the first model independent search for three-jet
hadronic resonances within multijet events in sqrt(s) =
1.96 TeV pp collisions at the Fermilab Tevatron using
the CDF II detector. Pair production of supersymmetric
gluinos and squarks with hadronic R-parity violating decays
is employed as an example of a new physics benchmark for
this signature. Selection criteria based on the kinematic
properties of an ensemble of jet combinations within each
event help to extract signal from copious QCD background. No
significant excess outside the top quark mass window is
observed in data with an integrated luminosity of
3.2 fb(-1). We place 95% confidence level limits on the
production cross section σ(pp → XX')×BR(gg →
3 jet + 3 jet) where X, X' = g, q, or q, with q, q
→ g + jet, as a function of gluino mass, in the range of
77 GeV/c2 to 240 GeV/c2.},
Doi = {10.1103/PhysRevLett.107.042001},
Key = {fds307843}
}
@article{fds307974,
Author = {Aaltonen, T and others},
Title = {First simultaneous measurement of the top quark mass in the
lepton + jets and dilepton channels at CDF},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {9},
Pages = {092005},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.092005},
Abstract = {We present a measurement of the mass of the top quark using
data corresponding to an integrated luminosity of 1.9fb-1 of
pp̄ collisions collected at s=1.96TeV with the CDF II
detector at Fermilab's Tevatron. This is the first
measurement of the top quark mass using top-antitop pair
candidate events in the lepton+jets and dilepton decay
channels simultaneously. We reconstruct two observables in
each channel and use a nonparametric kernel density
estimation technique to derive two-dimensional probability
density functions from simulated signal and background
samples. The observables are the top quark mass and the
invariant mass of two jets from the W decay in the
lepton+jets channel, and the top quark mass and the scalar
sum of transverse energy of the event in the dilepton
channel. We perform a simultaneous fit for the top quark
mass and the jet energy scale, which is constrained in situ
by the hadronic W boson mass. Using 332 lepton+jets
candidate events and 144 dilepton candidate events, we
measure the top quark mass to be Mtop=171.9±1.
7(stat+JES)±1.1(othersyst)GeV/c2=171.9±2.0GeV/c2. © 2009
The American Physical Society.},
Doi = {10.1103/PhysRevD.79.092005},
Key = {fds307974}
}
@article{fds310359,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ},
Title = {Flavor tagged time-dependent angular analysis of the Bs0
→J/ψφ decay and extraction of ΔΓs and the weak phase
φs in ATLAS},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052007},
Abstract = {A measurement of the Bs0→J/ψφ decay parameters, updated
to include flavor tagging is reported using 4.9fb-1 of
integrated luminosity collected by the ATLAS detector from
s=7TeV pp collisions recorded in 2011 at the LHC. The values
measured for the physical parameters are
φs=0.12±0.25(stat)±0.05(syst)radΔΓs=0.053±0.021(stat)±0.010(syst)ps-1Γs=0.677±0.007(stat)±0.004(syst)ps-1|A
(0)|2=0.220±0.008(stat)±0.009(syst)|A0(0)|2=0.529±0.006(stat)±0.012(syst)δ=3.89±0.47(stat)±0.11(syst)radwhere
the parameter ΔΓs is constrained to be positive. The
S-wave contribution was measured and found to be compatible
with zero. Results for φs and ΔΓs are also presented as
68% and 95% likelihood contours, which show agreement with
the Standard Model expectations.},
Doi = {10.1103/PhysRevD.90.052007},
Key = {fds310359}
}
@article{fds347521,
Author = {Kakati, B and Kotwal, A and Biswas, D and Sahu, S},
Title = {Fluconazole Resistant Candida Oesophagitis in
Immunocompetent Patients: Is Empirical Therapy
Justifiable?},
Journal = {Journal of clinical and diagnostic research :
JCDR},
Volume = {9},
Number = {12},
Pages = {DC16-DC18},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.7860/jcdr/2015/15171.6975},
Abstract = {<h4>Introduction</h4>C. albicans (Candida albicans) is the
foremost cause of fungal oesophagitis, however other species
such as Candida tropicalis, Candida krusei and Candida
stellatoidea have also been implicated to cause this
condition. Although, numerous studies have identified risk
factors for C. albicans oesophagitis, data for non- C.
albicans species is still sparse.<h4>Aim</h4>To determine
the aetiology of Candida oesophagitis in our medical centre
over a two year period. Additionally, to investigate
predisposing conditions for oesophageal candidiasis caused
by different Candida species.<h4>Material and
methods</h4>All consecutive patients posted for upper
gastrointestinal endoscopy at the endoscopy unit of a
tertiary care hospital in north India with findings
consistent with oesophagitis were screened for the presence
of Candida oesophagitis by performing KOH (potassium
hydroxide) examination and culture on SDA (Sabouraud's
dextrose agar). Antifungal susceptibility testing as per
CLSI guidelines was performed for fluconazole, a most common
empirically prescribed antifungal for the
condition.<h4>Results</h4>A total of 1868 patients with no
known immune-compromised condition underwent upper
gastroscopy at our centre during the study period. The
prevalence of Candida oesophagitis was 8.7% (n = 163). C.
albicans was recovered from majority of infections (52.1%),
followed by C. tropicalis (24%), C. parapsilosis (13.4%), C.
glabrata (6.9%) and C. krusei (3.6%). Alarmingly, among the
C. albicans isolates 8.6% were resistant to
fluconazole.<h4>Conclusion</h4>With rising reports of
antifungal drug resistance among the isolates of Candida
species, an increasing prevalence of this organism could
have an impact on the treatment of Candidal oesophagitis and
it should be approached with caution by the
clinician.},
Doi = {10.7860/jcdr/2015/15171.6975},
Key = {fds347521}
}
@article{fds356548,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP},
Title = {Fluctuations of anisotropic flow in Pb+Pb collisions at
√sNN = 5.02 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {1},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2020)051},
Abstract = {Multi-particle azimuthal cumulants are measured as a
function of centrality and transverse momentum using 470
μb−1 of Pb+Pb collisions at sNN = 5.02 TeV with the ATLAS
detector at the LHC. These cumulants provide information on
the event-by-event fluctuations of harmonic flow
coefficients vn and correlated fluctuations between two
harmonics vn and vm. For the first time, a non-zero
four-particle cumulant is observed for dipolar flow, v1. The
four-particle cumulants for elliptic flow, v2, and
triangular flow, v3, exhibit a strong centrality dependence
and change sign in ultra-central collisions. This sign
change is consistent with significant non-Gaussian
fluctuations in v2 and v3. The four-particle cumulant for
quadrangular flow, v4, is found to change sign in
mid-central collisions. Correlations between two harmonics
are studied with three- and four-particle mixed-harmonic
cumulants, which indicate an anti-correlation between v2 and
v3, and a positive correlation between v2 and v4. These
correlations decrease in strength towards central collisions
and either approach zero or change sign in ultra-central
collisions. To investigate the possible flow fluctuations
arising from intrinsic centrality or volume fluctuations,
the results are compared between two different event classes
used for centrality definitions. In peripheral and
mid-central collisions where the cumulant signals are large,
only small differences are observed. In ultra-central
collisions, the differences are much larger and transverse
momentum dependent. These results provide new information to
disentangle flow fluctuations from the initial and final
states, as well as new insights on the influence of
centrality fluctuations. [Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP01(2020)051},
Key = {fds356548}
}
@article{fds312244,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Forward-backward correlations and charged-particle azimuthal
distributions in pp interactions using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {7},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP07(2012)019},
Abstract = {Using inelastic proton-proton interactions at √s =900 GeV
and 7TeV, recorded by the ATLAS detector at the LHC,
measurements have been made of the correlations between
forward and backward charged-particle multiplicities and,
for the first time, between forward and backward
charged-particle summed transverse momentum. In addition,
jet-like structure in the events is studied by means of
azimuthal distributions of charged particles relative to the
charged particle with highest transverse momentum in a
selected kinematic region of the event. The results are
compared with predictions from tunes of the PYTHIA and
HERWIG++ Monte Carlo generators, which in most cases are
found to provide a reasonable description of the
data.},
Doi = {10.1007/JHEP07(2012)019},
Key = {fds312244}
}
@article{fds307728,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães Da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman De Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B and Clement, C and Clifft, RW},
Title = {Forward-backward correlations and charged-particle azimuthal
distributions in pp interactions using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {7},
Year = {2012},
url = {http://dx.doi.org/10.1007/JHEP07(1992)019},
Abstract = {Using inelastic proton-proton interactions at √s =900 GeV
and 7TeV, recorded by the ATLAS detector at the LHC,
measurements have been made of the correlations between
forward and backward charged-particle multiplicities and,
for the first time, between forward and backward
charged-particle summed transverse momentum. In addition,
jet-like structure in the events is studied by means of
azimuthal distributions of charged particles relative to the
charged particle with highest transverse momentum in a
selected kinematic region of the event. The results are
compared with predictions from tunes of the PYTHIA and
HERWIG++ Monte Carlo generators, which in most cases are
found to provide a reasonable description of the
data.},
Doi = {10.1007/JHEP07(1992)019},
Key = {fds307728}
}
@article{fds347538,
Author = {Patyal, S and Kotwal, A and Banarji, A and Gurunadh,
VS},
Title = {Frequency doubling technology and standard automated
perimetry in detection of glaucoma among glaucoma
suspects.},
Journal = {Medical journal, Armed Forces India},
Volume = {70},
Number = {4},
Pages = {332-337},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1016/j.mjafi.2013.09.002},
Abstract = {<h4>Background</h4>Frequency Doubling perimetry (FDT) has
been found to precede visual loss detected by standard
automated perimetry (SAP) by as much as four years and the
initial development of glaucomatous visual field loss as
measured by SAP was found to occur in regions that had
previously demonstrated abnormalities on FDT
testing.<h4>Methods</h4>A study on 55 glaucoma suspects
(determined as per American Academy Guidelines, Preferred
Practice Pattern, Oct 2010), was compared to 50 healthy
participants (HP). Both glaucoma suspects and HP underwent
SAP and FDT in random order. Only reliable fields were
compared.<h4>Results</h4>Mean deviation of FDT Matrix was
significantly lower than SAP SITA in suspect and healthy
group ; two devices showed significant correlation amongst
both groups (suspects p = 0.002, healthy p = 0.011).
Significant difference was found in PSD of SAP SITA and FDT
Matrix (p = 0.001) in the glaucoma suspect group, PSD of FDT
Matrix was significantly higher than PSD of SAP SITA in the
healthy group (p < 0.001). PSD of SAP SITA significantly
correlated with FDT Matrix PSD in glaucoma group (r = 0.579;
p = 0.001) but no significant correlation found in healthy
group (r = 0.153; p = 0.290). Percentages of normal test
locations significantly higher in FDT Matrix compared to SAP
SITA in glaucoma suspects and healthy participants.<h4>Conclusion</h4>FDT
correlates well with SAP and may be used for patients who
are unable to perform well and reliably with SAP but does
not show any features of earlier glaucoma changes in this
study.},
Doi = {10.1016/j.mjafi.2013.09.002},
Key = {fds347538}
}
@article{fds307671,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Further search for supersymmetry at √s=7TeV in final
states with jets, missing transverse momentum, and isolated
leptons with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.86.092002},
Abstract = {This work presents a new inclusive search for supersymmetry
(SUSY) by the ATLAS experiment at the LHC in proton-proton
collisions at a center-of-mass energy √s=7TeV in final
states with jets, missing transverse momentum and one or
more isolated electrons and/or muons. The search is based on
data from the full 2011 data-taking period, corresponding to
an integrated luminosity of 4.7fb-1. Single-lepton and
multilepton channels are treated together in one analysis.
An increase in sensitivity is obtained by simultaneously
fitting the number of events in statistically independent
signal regions, and the shapes of distributions within those
regions. A dedicated signal region is introduced to be
sensitive to decay cascades of SUSY particles with small
mass differences ("compressed SUSY"). Background
uncertainties are constrained by fitting to the
jet-multiplicity distribution in background control regions.
Observations are consistent with Standard Model
expectations, and limits are set or extended on a number of
SUSY models. © 2012 CERN.},
Doi = {10.1103/PhysRevD.86.092002},
Key = {fds307671}
}
@article{fds346192,
Author = {Agrawal, S and Deo, J and Verma, AK and Kotwal, A},
Title = {Geriatric health: need to make it an essential element of
primary health care.},
Journal = {Indian journal of public health},
Volume = {55},
Number = {1},
Pages = {25-29},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.4103/0019-557x.82540},
Abstract = {Within the next few decades, we will see an extraordinary
increase in the number of older people worldwide. The public
health benefit of preventive medicine in old age comes from
the compression of the time spent in dependency to a
minimum. A community-based, cross-sectional study was
conducted to assess the morbidity profile of the geriatric
population in a rural area of Maharashtra. A total of 214
subjects, of age 60 years and above, were examined. Data
were collected by structured interviews and clinical and
laboratory examinations. Out of the total of 214 subjects,
190 were suffering from some or the other diseases and the
major morbidities were visual (56%), musculoskeletal
(38.3%), respiratory (32.7%), and hypertension (28%). Anemia
was present in 62.6%, 5.61% had Diabetes Mellitus and 22.5%
were found to be overweight. The average morbidity load was
2.61. The rising morbidities clearly showed that a regular,
complete health checkup of the elderly should be embedded in
the essential elements of the Primary Health Care. This
would reduce the morbidity, improve the quality of life, and
facilitate 'Active Aging'.},
Doi = {10.4103/0019-557x.82540},
Key = {fds346192}
}
@article{fds307976,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Aurisano, A and Azfar, F and Azzurri, P and Badgett,
W and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung,
K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci,
MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway,
J},
Title = {Global search for new physics with 2.0fb-1 at
CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.79.011101},
Abstract = {Data collected in run II of the Fermilab Tevatron are
searched for indications of new electroweak-scale physics.
Rather than focusing on particular new physics scenarios,
CDF data are analyzed for discrepancies with the standard
model prediction. A model-independent approach (Vista)
considers gross features of the data, and is sensitive to
new large cross-section physics. Further sensitivity to new
physics is provided by two additional algorithms: a Bump
Hunter searches invariant mass distributions for "bumps"
that could indicate resonant production of new particles,
and the Sleuth procedure scans for data excesses at large
summed transverse momentum. This combined global search for
new physics in 2.0fb-1 of pp̄ collisions at s=1.96TeV
reveals no indication of physics beyond the standard model.
© 2009 The American Physical Society.},
Doi = {10.1103/PhysRevD.79.011101},
Key = {fds307976}
}
@article{fds346210,
Author = {Kotwal, A and Priya, R and Qadeer, I},
Title = {Goiter and other iodine deficiency disorders: A systematic
review of epidemiological studies to deconstruct the complex
web.},
Journal = {Archives of medical research},
Volume = {38},
Number = {1},
Pages = {1-14},
Year = {2007},
Month = {January},
url = {http://dx.doi.org/10.1016/j.arcmed.2006.08.006},
Abstract = {A systematic review of the available literature on goiter
and other iodine deficiency disorders (IDDs) was carried out
with the aim of analyzing available evidence and providing
inputs to the policy makers and program formulators
regarding the entire issue. The findings point to major
issues such as the following: methodological issues in
epidemiology of goiter and other iodine deficiency disorders
(IDDs); lacunae in causal linkages; inadequate attention to
multicausality; flawed assessment of the impact of
intervention, i.e., iodized salt; and harmful effects of
iodine not given due cognizance. Most of the research to
date has been unidirectional and does not provide
comprehensive data on all aspects of IDDs. To further
compound the issue, many independent researchers, on finding
something different from the existing dominant paradigm
(iodized salt as panacea for goiter) have tended to ignore
these in their final conclusions and recommendations. Thus,
evidence from this systematic review demonstrates enough
basis to start a debate on the entire issue, recognizing
opposing research findings while continuing with the present
strategy. This imposes specific problems and necessitates
area-specific solutions instead of a universal solution,
which apart from being less effective may be harmful in the
long run.},
Doi = {10.1016/j.arcmed.2006.08.006},
Key = {fds346210}
}
@article{fds346183,
Author = {Anargh, V and Singh, H and Kulkarni, A and Kotwal, A and Mahen,
A},
Title = {Hand hygiene practices among health care workers (HCWs) in a
tertiary care facility in Pune.},
Journal = {Medical journal, Armed Forces India},
Volume = {69},
Number = {1},
Pages = {54-56},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.08.011},
Abstract = {<h4>Background</h4>Improper hand hygiene by healthcare
workers (HCWs) is responsible for about 40% of nosocomial
infections resulting in prolonged illnesses, hospital stays,
long-term disability and unexpected high costs on patients
and their families, and also lead to a massive additional
financial burden on the health-care system.<h4>Objective</h4>To
assess knowledge and practices regarding hand hygiene among
HCWs of a tertiary health care facility.<h4>Methods</h4>A
cross sectional, questionnaire and observation based study
was carried out in a tertiary care health care facility in
Pune. Based on sample size calculations, 100 HCWs working in
medical and surgical wards were studied.<h4>Results</h4>The
proportion knowledgeable about hand hygiene practices was
85% and 73% HCWs were of the belief that unclean hands are
an important route of cross transmission. WHO guidelines
regarding procedure were being followed by 90% for hand
washing with soap and water and 64% for alcohol based rubs.
Majority preferred hand washing with soap and water over
hand rubbing with alcohol based solutions. 21% of HCWs were
missing hand hygiene opportunities 1 in 5 times. Heavy
workload (38%), non availability (52%) and inaccessibility
(9%) of hand hygiene facilities were the common reasons for
non-compliance. Availability of 'one time use paper towels'
was low (12%).<h4>Conclusion</h4>Inadequate compliance
despite knowledge and false sense of security by alcohol
based rubs was seen. A multi disciplinary, multifaceted
approach is required to tackle issues of
non-compliance.},
Doi = {10.1016/j.mjafi.2012.08.011},
Key = {fds346183}
}
@article{fds331389,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Bolton,
TA and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and De,
K and De Jong and SJ and Demarteau, M and Demina, R and Demine, P and Denisov,
D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot,
L},
Title = {Hard single diffraction in p̄ p collisions at √s = 630
and 1800 GeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {531},
Number = {1-2},
Pages = {52-60},
Publisher = {Elsevier BV},
Year = {2002},
Month = {April},
url = {http://dx.doi.org/10.1016/S0370-2693(02)01364-3},
Abstract = {Using the DØ detector, we have studied events produced in
p-p collisions that contain large forward regions with very
little energy deposition ("rapidity gaps") and concurrent
jet production at center-of-mass energies of √s = 630 and
1800 GeV. The fraction of events with forward or central
jets associated with rapidity gaps is compared to
predictions for hard diffraction. We also extract the
momentum loss for scattered protons in such
processes.},
Doi = {10.1016/S0370-2693(02)01364-3},
Key = {fds331389}
}
@article{fds346161,
Author = {Abada, A and Abbrescia, M and AbdusSalam, SS and Abdyukhanov, I and Abelleira Fernandez and J and Abramov, A and Aburaia, M and Acar, AO and Adzic, PR and Agrawal, P and Aguilar-Saavedra, JA and Aguilera-Verdugo, JJ and Aiba, M and Aichinger, I and Aielli, G and Akay, A and Akhundov, A and Aksakal, H and Albacete, JL and Albergo, S and Alekou, A and Aleksa, M and Aleksan, R and Alemany Fernandez and RM and Alexahin, Y and Alía, RG and Alioli, S and Alipour Tehrani and N and Allanach, BC and Allport, PP and Altınlı, M and Altmannshofer, W and Ambrosio, G and Amorim, D and Amstutz, O and Anderlini, L and Andreazza,
A and Andreini, M and Andriatis, A and Andris, C and Andronic, A and Angelucci, M and Antinori, F and Antipov, SA and Antonelli, M and Antonello, M and Antonioli, P and Antusch, S and Anulli, F and Apolinário, L and Apollinari, G and Apollonio, A and Appelö, D and Appleby, RB and Apyan, A and Arbey, A and Arbuzov, A and Arduini, G and Arı, V and Arias, S and Armesto, N and Arnaldi, R and Arsenyev, SA and Arzeo, M and Asai, S and Aslanides, E and Aßmann, RW and Astapovych, D and Atanasov, M and Atieh, S and Attié, D and Auchmann, B and Audurier, A and Aull, S and Aumon, S and Aune, S and Avino, F and Avrillaud, G and Aydın,
G and Azatov, A and Azuelos, G and Azzi, P and Azzolini, O and Azzurri, P and Bacchetta, N and Bacchiocchi, E and Bachacou, H and Baek, YW and Baglin,
V and Bai, Y and Baird, S and Baker, MJ and Baldwin, MJ and Ball, AH and Ballarino, A and Banerjee, S and Barber, DP and Barducci, D and Barjhoux, P},
Title = {HE-LHC: The High-Energy Large Hadron Collider: Future
Circular Collider Conceptual Design Report Volume
4},
Journal = {European Physical Journal: Special Topics},
Volume = {228},
Number = {5},
Pages = {1109-1382},
Year = {2019},
Month = {July},
url = {http://dx.doi.org/10.1140/epjst/e2019-900088-6},
Abstract = {In response to the 2013 Update of the European Strategy for
Particle Physics (EPPSU), the Future Circular Collider (FCC)
study was launched as a world-wide international
collaboration hosted by CERN. The FCC study covered an
energy-frontier hadron collider (FCC-hh), a
highest-luminosity high-energy lepton collider (FCC-ee), the
corresponding 100 km tunnel infrastructure, as well as the
physics opportunities of these two colliders, and a
high-energy LHC, based on FCC-hh technology. This document
constitutes the third volume of the FCC Conceptual Design
Report, devoted to the hadron collider FCC-hh. It summarizes
the FCC-hh physics discovery opportunities, presents the
FCC-hh accelerator design, performance reach, and staged
operation plan, discusses the underlying technologies, the
civil engineering and technical infrastructure, and also
sketches a possible implementation. Combining ingredients
from the Large Hadron Collider (LHC), the high-luminosity
LHC upgrade and adding novel technologies and approaches,
the FCC-hh design aims at significantly extending the energy
frontier to 100 TeV. Its unprecedented centre-of-mass
collision energy will make the FCC-hh a unique instrument to
explore physics beyond the Standard Model, offering great
direct sensitivity to new physics and discoveries.},
Doi = {10.1140/epjst/e2019-900088-6},
Key = {fds346161}
}
@article{fds346195,
Author = {Kotwal, A and Taneja, D},
Title = {Health Care Workers and Universal Precautions: Perceptions
and Determinants of Non-compliance.},
Journal = {Indian journal of community medicine : official publication
of Indian Association of Preventive & Social
Medicine},
Volume = {35},
Number = {4},
Pages = {526-528},
Year = {2010},
Month = {October},
url = {http://dx.doi.org/10.4103/0970-0218.74373},
Doi = {10.4103/0970-0218.74373},
Key = {fds346195}
}
@article{fds352787,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Higgs boson production cross-section measurements and their
EFT interpretation in the 4 ℓ decay channel at √s=
13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8227-9},
Abstract = {Higgs boson properties are studied in the four-lepton decay
channel (where lepton = e, μ) using 139 fb - 1 of
proton–proton collision data recorded at s=13 TeV by the
ATLAS experiment at the Large Hadron Collider. The inclusive
cross-section times branching ratio for H→ ZZ∗ decay is
measured to be 1.34 ± 0.12 pb for a Higgs boson with
absolute rapidity below 2.5, in good agreement with the
Standard Model prediction of 1.33 ± 0.08 pb. Cross-sections
times branching ratio are measured for the main Higgs boson
production modes in several exclusive phase-space regions.
The measurements are interpreted in terms of coupling
modifiers and of the tensor structure of Higgs boson
interactions using an effective field theory approach.
Exclusion limits are set on the CP-even and CP-odd ‘beyond
the Standard Model’ couplings of the Higgs boson to vector
bosons, gluons and top quarks.},
Doi = {10.1140/epjc/s10052-020-8227-9},
Key = {fds352787}
}
@article{fds307578,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu,
A},
Title = {Higgs boson studies at the Tevatron},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.88.052014},
Abstract = {We combine searches by the CDF and D0 Collaborations for the
standard model Higgs boson with mass in the range 90-200
GeV/c2 produced in the gluon-gluon fusion, WH, ZH, tt̄H,
and vector boson fusion processes, and decaying in the
H→bb̄, H→W+W-, H→ZZ, H→τ+τ-, and H→γγ modes.
The data correspond to integrated luminosities of up to 10
fb-1 and were collected at the Fermilab Tevatron in pp̄
collisions at √s=1.96 TeV. The searches are also
interpreted in the context of fermiophobic and fourth
generation models. We observe a significant excess of events
in the mass range between 115 and 140 GeV/c2. The local
significance corresponds to 3.0 standard deviations at
mH=125 GeV/c2, consistent with the mass of the Higgs boson
observed at the LHC, and we expect a local significance of
1.9 standard deviations. We separately combine searches for
H→bb̄, H→W +W-, H→τ+τ-, and H→γγ. The observed
signal strengths in all channels are consistent with the
presence of a standard model Higgs boson with a mass of 125
GeV/c2. © 2013 American Physical Society.},
Doi = {10.1103/PhysRevD.88.052014},
Key = {fds307578}
}
@article{fds362575,
Author = {Dawson, S and Gritsan, A and Logan, H and Qian, J and Tully, C and Kooten,
RV and Ajaib, A and Anastassov, A and Anderson, I and Asner, D and Bake, O and Barger, V and Barklow, T and Batell, B and Battaglia, M and Berge, S and Blondel, A and Bolognesi, S and Brau, J and Brownson, E and Cahill-Rowley, M and Calancha-Paredes, C and Chen, C-Y and Chou, W and Clare, R and Cline, D and Craig, N and Cranmer, K and Gruttola, MD and Elagin, A and Essig, R and Everett, L and Feng, E and Fujii, K and Gainer,
J and Gao, Y and Gogoladze, I and Gori, S and Goncalo, R and Graf, N and Grojean, C and Guindon, S and Haber, H and Han, T and Hanson, G and Harnik,
R and Heinemeyer, S and Heintz, U and Hewett, J and Ilchenko, Y and Ishikawa, A and Ismail, A and Jain, V and Janot, P and Kanemura, S and Kawada, S and Kehoe, R and Klute, M and Kotwal, A and Krueger, K and Kukartsev, G and Kumar, K and Kunkle, J and Kurata, M and Lewis, I and Li,
Y and Linssen, L and Lipeles, E and Lipton, R and Liss, T and List, J and Liu,
T and Liu, Z and Low, I and Ma, T and Mackenzie, P and Mellado, B and Melnikov, K and Miyamoto, A and Moortgat-Pick, G and Mourou, G and Narain, M and Neal, H and Nielsen, J and Okada, N and Okawa, H and Olsen,
J and Ono, H and Onyisi, P and Parashar, N and Peskin, M and Petriello, F and Plehn, T and Pollard, C and Potter, C and Prokofiev, K and Rauch, M and Rizzo, T and Robens, T and Rodriguez, V and Roloff, P and Ruiz, R and Sanz,
V and Sayre, J and Shafi, Q and Shaughnessy, G and Sher, M and Simon, F and Solyak, N and Strube, J and Stupak, J and Su, S and Suehara, T and Tanabe,
T and Tajima, T and Telnov, V and Tian, J and Thomas, S and Thomson, M and Tsumura, K and Un, C and Velasco, M and Wagner, C and Wang, S and Watanuki,
S and Weiglein, G and Whitbeck, A and Yagyu, K and Yao, W and Yokoya, H and Zenz, S and Zerwas, D and Zhang, Y and Zhou, Y},
Title = {Higgs Working Group Report of the Snowmass 2013 Community
Planning Study},
Year = {2013},
Month = {October},
Abstract = {This report summarizes the work of the Energy Frontier Higgs
Boson working group of the 2013 Community Summer Study
(Snowmass). We identify the key elements of a precision
Higgs physics program and document the physics potential of
future experimental facilities as elucidated during the
Snowmass study. We study Higgs couplings to gauge boson and
fermion pairs, double Higgs production for the Higgs
self-coupling, its quantum numbers and $CP$-mixing in Higgs
couplings, the Higgs mass and total width, and prospects for
direct searches for additional Higgs bosons in extensions of
the Standard Model. Our report includes projections of
measurement capabilities from detailed studies of the
Compact Linear Collider (CLIC), a Gamma-Gamma Collider, the
International Linear Collider (ILC), the Large Hadron
Collider High-Luminosity Upgrade (HL-LHC), Very Large Hadron
Colliders up to 100 TeV (VLHC), a Muon Collider, and a
Triple-Large Electron Positron Collider (TLEP).},
Key = {fds362575}
}
@article{fds346211,
Author = {Kotwal, J and Apte, CV and Kotwal, A and Mukherjee, B and Jayaram,
J},
Title = {High altitude: a hypercoagulable state: results of a
prospective cohort study.},
Journal = {Thrombosis research},
Volume = {120},
Number = {3},
Pages = {391-397},
Year = {2007},
Month = {January},
url = {http://dx.doi.org/10.1016/j.thromres.2006.09.013},
Doi = {10.1016/j.thromres.2006.09.013},
Key = {fds346211}
}
@article{fds356752,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and AlvarezGonzalez, B and ÁlvarezPiqueras, D and Alviggi, MG and Amadio, BT and AmaralCoutinho, Y and Amelung, C and Amidei, D and AmorDosSantos, SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and AperioBella, L and Arabidze, G and Arai, Y and Araque,
JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik,
M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {High-ET isolated-photon plus jets production in
pp collisions at s=8 TeV with the ATLAS detector},
Journal = {Nuclear Physics B},
Volume = {918},
Pages = {257-316},
Year = {2017},
Month = {May},
url = {http://dx.doi.org/10.1016/j.nuclphysb.2017.03.006},
Abstract = {The dynamics of isolated-photon plus one-, two- and
three-jet production in pp collisions at a centre-of-mass
energy of 8 TeV are studied with the ATLAS detector at the
LHC using a data set with an integrated luminosity of 20.2
fb−1. Measurements of isolated-photon plus jets cross
sections are presented as functions of the photon and jet
transverse momenta. The cross sections as functions of the
azimuthal angle between the photon and the jets, the
azimuthal angle between the jets, the photon–jet invariant
mass and the scattering angle in the photon–jet
centre-of-mass system are presented. The pattern of QCD
radiation around the photon and the leading jet is
investigated by measuring jet production in an annular
region centred on each object; enhancements are observed
around the leading jet with respect to the photon in the
directions towards the beams. The experimental measurements
are compared to several different theoretical calculations,
and overall a good description of the data is
found.},
Doi = {10.1016/j.nuclphysb.2017.03.006},
Key = {fds356752}
}
@article{fds362779,
Author = {CDF Collaboration†‡, and Aaltonen, T and Amerio, S and Amidei,
D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland,
KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes,
RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori,
M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen,
AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles,
E and Lister, A and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti,
P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian,
C and Miao, T and Michielin, E and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet,
M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, K and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang, SM and Waters,
D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfmeister, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli,
S},
Title = {High-precision measurement of the W boson mass with
the CDF II detector.},
Journal = {Science (New York, N.Y.)},
Volume = {376},
Number = {6589},
Pages = {170-176},
Year = {2022},
Month = {April},
url = {http://dx.doi.org/10.1126/science.abk1781},
Abstract = {The mass of the <i>W</i> boson, a mediator of the weak force
between elementary particles, is tightly constrained by the
symmetries of the standard model of particle physics. The
Higgs boson was the last missing component of the model.
After observation of the Higgs boson, a measurement of the
<i>W</i> boson mass provides a stringent test of the model.
We measure the <i>W</i> boson mass, <i>M<sub>W</sub></i>,
using data corresponding to 8.8 inverse femtobarns of
integrated luminosity collected in proton-antiproton
collisions at a 1.96 tera-electron volt center-of-mass
energy with the CDF II detector at the Fermilab Tevatron
collider. A sample of approximately 4 million <i>W</i> boson
candidates is used to obtain <b>[Formula: see text]</b>, the
precision of which exceeds that of all previous measurements
combined (stat, statistical uncertainty; syst, systematic
uncertainty; MeV, mega-electron volts; <i>c</i>, speed of
light in a vacuum). This measurement is in significant
tension with the standard model expectation.},
Doi = {10.1126/science.abk1781},
Key = {fds362779}
}
@article{fds332354,
Author = {Abbott, B and Abdesselam, A and Abolins, M and Abramov, V and Acharya,
BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and Del
Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S},
Title = {High-[Formula Presented] jets in [Formula Presented]
collisions at [Formula Presented] and 1800
GeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {64},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2001},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.64.032003},
Abstract = {Results are presented from analyses of jet data produced in
[Formula Presented] collisions at [Formula Presented] and
1800 GeV collected with the DØ detector during the
1994–1995 Fermilab Tevatron Collider run. We discuss the
details of detector calibration, and jet selection criteria
in measurements of various jet production cross sections at
[Formula Presented] and 1800 GeV. The inclusive jet cross
sections, the dijet mass spectrum, the dijet angular
distributions, and the ratio of inclusive jet cross sections
at [Formula Presented] and 1800 GeV are compared to
next-to-leading-order QCD predictions. The order [Formula
Presented] calculations are in good agreement with the data.
We also use the data at [Formula Presented] GeV to rule out
models of quark compositeness with a contact interaction
scale less than [Formula Presented] TeV at the [Formula
Presented] confidence level. © 2001 The American Physical
Society.},
Doi = {10.1103/PhysRevD.64.032003},
Key = {fds332354}
}
@article{fds347532,
Author = {Sharma, M and Biswas, D and Kotwal, A and Thakuria, B and Kakati, B and Chauhan, BS and Patras, A},
Title = {Ibuprofen-mediated reversal of fluconazole resistance in
clinical isolates of Candida.},
Journal = {Journal of clinical and diagnostic research :
JCDR},
Volume = {9},
Number = {1},
Pages = {DC20-DC22},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.7860/jcdr/2015/10094.5494},
Abstract = {<h4>Introduction</h4>In view of the increasing prevalence of
invasive Candidiasis in today's health-care scenario and the
emergence of fluconazole resistance among clinical isolates
of Candida, we sought to determine if Ibuprofen could elicit
a reversal of fluconazole resistance and thereby offer a
potential therapeutic breakthrough in fluconazole-resistant
Candidiasis.<h4>Materials and methods</h4>We selected 69
clinical isolates of Candida, which demonstrated an MIC of
>32 μg/ml for fluconazole, and subjected them to broth
microdilution in presence and absence of
Ibuprofen.<h4>Results</h4>Forty two of the 69 isolates
(60.9%) demonstrated reversal of Fluconazole resistance with
concomitant use of Ibuprofen. This was characterized by
significant species-wise variation (p=0.00008), with all the
C. albicans isolates and none of the C. glabrata isolates
demonstrating such reversal. Only 22.2% and 37.7% of C.
krusei and C. tropicalis isolates respectively showed
Ibuprofen-mediated reversal of Fluconazole
resistance.<h4>Conclusion</h4>Since Ibuprofen is a known
efflux pump inhibitor, our findings hint at the possible
mechanism of Fluconazole resistance in most of our Candida
isolates and suggest a potential therapeutic alternative
that could be useful in the majority of Fluconazole-resistant
clinical isolates of Candida.},
Doi = {10.7860/jcdr/2015/10094.5494},
Key = {fds347532}
}
@article{fds321138,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas,
AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus,
M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Bedikian, S and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger,
N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black,
CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet,
D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli,
R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole,
B},
Title = {Identification and energy calibration of hadronically
decaying tau leptons with the ATLAS experiment in pp
collisions at [Formula: see text][Formula: see
text].},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {303},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3500-z},
Abstract = {This paper describes the trigger and offline reconstruction,
identification and energy calibration algorithms for
hadronic decays of tau leptons employed for the data
collected from <i>pp</i> collisions in 2012 with the ATLAS
detector at the LHC center-of-mass energy [Formula: see
text] [Formula: see text]. The performance of these
algorithms is measured in most cases with [Formula: see
text] decays to tau leptons using the full 2012 dataset,
corresponding to an integrated luminosity of 20.3
fb[Formula: see text]. An uncertainty on the offline
reconstructed tau energy scale of 2-4 %, depending on
transverse energy and pseudorapidity, is achieved using two
independent methods. The offline tau identification
efficiency is measured with a precision of 2.5 % for
hadronically decaying tau leptons with one associated track,
and of 4 % for the case of three associated tracks,
inclusive in pseudorapidity and for a visible transverse
energy greater than 20 [Formula: see text]. For hadronic tau
lepton decays selected by offline algorithms, the tau
trigger identification efficiency is measured with a
precision of 2-8 %, depending on the transverse energy. The
performance of the tau algorithms, both offline and at the
trigger level, is found to be stable with respect to the
number of concurrent proton-proton interactions and has
supported a variety of physics results using hadronically
decaying tau leptons at ATLAS.},
Doi = {10.1140/epjc/s10052-015-3500-z},
Key = {fds321138}
}
@article{fds348983,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa,
JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan,
AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini,
D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni,
LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret,
MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini,
M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney,
RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castelijn, R and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito,
L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Identification and rejection of pile-up jets at high
pseudorapidity with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {9},
Pages = {580},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5081-5},
Abstract = {The rejection of forward jets originating from additional
proton-proton interactions (pile-up) is crucial for a
variety of physics analyses at the LHC, including Standard
Model measurements and searches for physics beyond the
Standard Model. The identification of such jets is
challenging due to the lack of track and vertex information
in the pseudorapidity range | η | > 2.5 . This paper
presents a novel strategy for forward pile-up jet tagging
that exploits jet shapes and topological jet correlations in
pile-up interactions. Measurements of the per-jet tagging
efficiency are presented using a data set of 3.2 fb - 1 of
proton-proton collisions at a centre-of-mass energy of 13
TeV collected with the ATLAS detector. The fraction of
pile-up jets rejected in the range 2.5 < | η | < 4.5 is
estimated in simulated events with an average of 22
interactions per bunch-crossing. It increases with jet
transverse momentum and, for jets with transverse momentum
between 20 and 50 GeV, it ranges between 49% and 67% with an
efficiency of 85% for selecting hard-scatter jets. A case
study is performed in Higgs boson production via the
vector-boson fusion process, showing that these techniques
mitigate the background growth due to additional
proton-proton interactions, thus enhancing the reach for
such signatures.},
Doi = {10.1140/epjc/s10052-017-5081-5},
Key = {fds348983}
}
@article{fds356567,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
Title = {Identification of boosted Higgs bosons decaying into b-quark
pairs with the ATLAS detector at 13 TeV},
Journal = {European Physical Journal C},
Volume = {79},
Number = {10},
Year = {2019},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7335-x},
Abstract = {This paper describes a study of techniques for identifying
Higgs bosons at high transverse momenta decaying into
bottom-quark pairs, H→ bb¯ , for proton–proton
collision data collected by the ATLAS detector at the Large
Hadron Collider at a centre-of-mass energy s=13 TeV. These
decays are reconstructed from calorimeter jets found with
the anti-ktR= 1.0 jet algorithm. To tag Higgs bosons, a
combination of requirements is used: b-tagging of R= 0.2
track-jets matched to the large-R calorimeter jet, and
requirements on the jet mass and other jet substructure
variables. The Higgs boson tagging efficiency and
corresponding multijet and hadronic top-quark background
rejections are evaluated using Monte Carlo simulation.
Several benchmark tagging selections are defined for
different signal efficiency targets. The modelling of the
relevant input distributions used to tag Higgs bosons is
studied in 36 fb- 1 of data collected in 2015 and 2016
using g→ bb¯ and Z(→ bb¯) γ event selections in data.
Both processes are found to be well modelled within the
statistical and systematic uncertainties.},
Doi = {10.1140/epjc/s10052-019-7335-x},
Key = {fds356567}
}
@article{fds347518,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister,
I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman,
JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn,
AP},
Title = {Identification of boosted, hadronically decaying W
bosons and comparisons with ATLAS data taken at [Formula:
see text] TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {154},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3978-z},
Abstract = {This paper reports a detailed study of techniques for
identifying boosted, hadronically decaying <i>W</i> bosons
using 20.3 fb[Formula: see text] of proton-proton collision
data collected by the ATLAS detector at the LHC at a
centre-of-mass energy [Formula: see text]. A range of
techniques for optimising the signal jet mass resolution are
combined with various jet substructure variables. The
results of these studies in Monte Carlo simulations show
that a simple pairwise combination of groomed jet mass and
one substructure variable can provide a 50 % efficiency for
identifying <i>W</i> bosons with transverse momenta larger
than 200 GeV while maintaining multijet background
efficiencies of 2-4 % for jets with the same transverse
momentum. These signal and background efficiencies are
confirmed in data for a selection of tagging
techniques.},
Doi = {10.1140/epjc/s10052-016-3978-z},
Key = {fds347518}
}
@article{fds308169,
Author = {Kotwal, AV and Gerberich, HK and Hays, C},
Title = {Identification of cosmic rays using drift chamber hit
timing},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {506},
Number = {1-2},
Pages = {110-118},
Publisher = {Elsevier BV},
Year = {2003},
Month = {June},
url = {http://dx.doi.org/10.1016/S0168-9002(03)01371-8},
Abstract = {Identification of cosmic rays was discussed. Drift chamber
hit timing method was used. The central outer tracker (COT)
tracks as cosmic rays were studied and their direction of
propagation and time of incidence were also
measured.},
Doi = {10.1016/S0168-9002(03)01371-8},
Key = {fds308169}
}
@article{fds321126,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Identification of high transverse momentum top quarks in pp
collisions at √s= 8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {6},
Publisher = {Springer Nature},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2016)093},
Abstract = {This paper presents studies of the performance of several
jet-substructure techniques, which are used to identify
hadronically decaying top quarks with high transverse
momentum contained in large-radius jets. The efficiency of
identifying top quarks is measured using a sample of
top-quark pairs and the rate of wrongly identifying jets
from other quarks or gluons as top quarks is measured using
multijet events collected with the ATLAS experiment in 20.3
fb−1of 8 TeV proton-proton collisions at the Large Hadron
Collider. Predictions from Monte Carlo simulations are found
to provide an accurate description of the performance. The
techniques are compared in terms of signal efficiency and
background rejection using simulations, covering a larger
range in jet transverse momenta than accessible in the
dataset. Additionally, a novel technique is developed that
is optimized to reconstruct top quarks in events with many
jets.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP06(2016)093},
Key = {fds321126}
}
@article{fds307589,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
Title = {Improved luminosity determination in pp collisions at
[Formula: see text] using the ATLAS detector at the
LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {8},
Pages = {2518},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2518-3},
Abstract = {The luminosity calibration for the ATLAS detector at the LHC
during <i>pp</i> collisions at [Formula: see text] in 2010
and 2011 is presented. Evaluation of the luminosity scale is
performed using several luminosity-sensitive detectors, and
comparisons are made of the long-term stability and accuracy
of this calibration applied to the <i>pp</i> collisions at
[Formula: see text]. A luminosity uncertainty of [Formula:
see text] is obtained for the 47 pb<sup>-1</sup> of data
delivered to ATLAS in 2010, and an uncertainty of [Formula:
see text] is obtained for the 5.5 fb<sup>-1</sup> delivered
in 2011.},
Doi = {10.1140/epjc/s10052-013-2518-3},
Key = {fds307589}
}
@article{fds184837,
Author = {A.V. Kotwal and T. Aaltonen et al [CDF Collaboration]},
Title = {Improved Search for a Higgs Boson Produced in Association
with Z->l+l- in proton antiproton Collisions at sqrt(s) =
1.96 TeV},
Journal = {Physical Review Letters},
Year = {2010},
Month = {Fall},
Key = {fds184837}
}
@article{fds307893,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco,
SD and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shekhar, R and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki, M and Denis,
RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini,
N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez,
F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang,
T},
Title = {Improved search for a Higgs boson produced in association
with Z→l+l- in pp̄ collisions at
√s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {105},
Number = {25},
Pages = {251802},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.251802},
Abstract = {We search for the standard model Higgs boson produced with a
Z boson in 4.1fb⊃-1 of integrated luminosity collected
with the CDF II detector at the Tevatron. In events
consistent with the decay of the Higgs boson to a
bottom-quark pair and the Z boson to electrons or muons, we
set 95% credibility level upper limits on the ZH production
cross section multiplied by the H→bb̄ branching ratio.
Improved analysis methods enhance signal sensitivity by 20%
relative to previous searches. At a Higgs boson mass of
115GeV/c2 we set a limit of 5.9 times the standard model
cross section. © 2010 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.105.251802},
Key = {fds307893}
}
@article{fds337272,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Bolton,
TA and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and De,
K and Jong, SJD and Demarteau, M and Demina, R and Demine, P and Denisov,
D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Duperrin, A and Dyshkant, A and Edmunds, D and Ellison, J and Eltzroth,
JT and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
T and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Fox, H and Frame, KC and Fu,
S and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
R and Ginther, G and Gómez, B and Goncharov, PI and Gordon, H and Goss,
LT and Gounder, K and Goussiou, A and Graf, N and Grannis, PD and Green,
JA and Greenlee, H and Greenwood, ZD and Grinstein, S and Groer, L and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Huang, Y and Iashvili, I and Illingworth, R and Ito, AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jöstlein, H and Juste, A and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Kehoe, R and Khanov, A and Kharchilava,
A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kothari, B and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Lee, WM and Leflat, A and Leggett, C and Lehner, F and Leonidopoulos, C and Li, J and Li, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann,
J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AKA and Madaras, RJ and Malyshev, VL and Manankov, V and Mao,
HS and Marshall, T and Martin, MI and Mayorov, AA and McCarthy, R and McMahon, T and Melanson, HL and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov, N and Mondal,
NK and Montgomery, HE and Moore, RW and Mostafa, M and Motta, HD and Mutaf,
Y and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret, JP and Nomerotski, A and Nunnemann, T and O'Neil,
D and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Peters, O and Pétroff, P and Piegaia, R and Pope, BG and Popkov, E and Prosper, HB and Protopopescu,
S and Przybycien, MB and Qian, J and Raja, R and Rajagopalan, S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Ridel, M and Rijssenbeek, M and Rizatdinova, F and Rockwell, T and Roco, M and Royon,
C and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Sajot, G and Santoro, A and Sawyer, L and Schamberger, RD and Schellman,
H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Song, Y and Sorín,
V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stoker, D and Stolin, V and Stone, A and Stoyanova, DA and Strang, MA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and Vaniev, V and Kooten, RV and Varelas, N and Vertogradov,
LS and Villeneuve-Seguier, F and Volkov, AA and Vorobiev, AP and Wahl,
HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wijngaarden,
DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Xu, Q and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Zanabria, M and Zhang, X and Zheng, H and Zhou, B and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi,
V and Zverev, EG and Zylberstejn, A},
Title = {Improved W boson mass measurement with the DØ
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {66},
Number = {1 II},
Pages = {120011-1200118},
Publisher = {American Physical Society (APS)},
Year = {2002},
url = {http://dx.doi.org/10.1103/PhysRevD.66.012001},
Abstract = {We have measured the W boson mass using the DØ detector and
a data sample of 82 pb-1 from the Fermilab Tevatron
collider. This measurement uses W→eν decays, where the
electron is close to a boundary of a central electromagnetic
calorimeter module. Such "edge" electrons have not been used
in any previous DØ analysis, and represent a 14% increase
in the W boson sample size. For these electrons, new
response and resolution parameters are determined, and
revised backgrounds and underlying event energy flow
measurements are made. When the current measurement is
combined with previous DØ W boson mass measurements, we
obtain MW=80.483±0.084 GeV. The 8% improvement from the
previous DØ measurement is primarily due to the improved
determination of the response parameters for non-edge
electrons using the sample of Z bosons with non-edge and
edge electrons.},
Doi = {10.1103/PhysRevD.66.012001},
Key = {fds337272}
}
@article{fds356627,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {In situ calibration of large-radius jet energy and mass in
13 TeV proton–proton collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {2},
Year = {2019},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6632-8},
Abstract = {The response of the ATLAS detector to large-radius jets is
measured in situ using 36.2 fb- 1 of s=13 TeV proton–proton
collisions provided by the LHC and recorded by the ATLAS
experiment during 2015 and 2016. The jet energy scale is
measured in events where the jet recoils against a reference
object, which can be either a calibrated photon, a
reconstructed Z boson, or a system of well-measured
small-radius jets. The jet energy resolution and a
calibration of forward jets are derived using dijet balance
measurements. The jet mass response is measured with two
methods: using mass peaks formed by W bosons and top quarks
with large transverse momenta and by comparing the jet mass
measured using the energy deposited in the calorimeter with
that using the momenta of charged-particle tracks. The
transverse momentum and mass responses in simulations are
found to be about 2–3% higher than in data. This
difference is adjusted for with a correction factor. The
results of the different methods are combined to yield a
calibration over a large range of transverse momenta (pT).
The precision of the relative jet energy scale is 1–2% for
200GeV<pT<2TeV, while that of the mass scale is 2–10%. The
ratio of the energy resolutions in data and simulation is
measured to a precision of 10–15% over the same pT
range.},
Doi = {10.1140/epjc/s10052-019-6632-8},
Key = {fds356627}
}
@article{fds308217,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, H and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G},
Title = {Inclusive jet cross section in p̄p collisions at √ = 1.8
TeV},
Journal = {Physical Review Letters},
Volume = {82},
Number = {12},
Pages = {2451-2456},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.2451},
Abstract = {We have made a precise measurement of the central inclusive
jet cross section at √s = 1.8 TeV. The measurement is
based on an integrated luminosity of 92pb-1 collected at the
Fermilab Tevatron p̄p Collider with the D0 detector. The
cross section, reported as a function of jet transverse
energy (ET ≥ 60 GeV) in the pseudorapidity interval |±|
≤ 0.5, is in good agreement with predictions from
next-to-leading order quantum chromodynamics. © 1999 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.82.2451},
Key = {fds308217}
}
@article{fds308182,
Author = {Abbott, B and Abdesselam, A and Abolins, M and Abramov, V and Acharya,
BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Davis, GA and Davis, K and De, K and Del
Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
T and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin, R and Ginther,
G and Gómez, B and Gómez, G and Goncharov, PI and González Solís,
JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein,
S and Groer, L and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Illingworth, R and Ito, AS and Jaffré, M and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov,
VE and Landsberg, G and Leflat, A and Leggett, C and Lehner, F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin, MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald, J and McMahon, T and Melanson, HL and Meng,
XC and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea,
D and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Nunnemann, T and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu,
S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan, S and Ramberg,
E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon,
J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev,
V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yip,
K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
EG and Zylberstejn, A and D0 Collaboration},
Title = {Inclusive jet production in pp(macro) collisions.},
Journal = {Physical review letters},
Volume = {86},
Number = {9},
Pages = {1707-1712},
Year = {2001},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.86.1707},
Abstract = {We report a new measurement of the pseudorapidity (eta) and
transverse-energy ( E(T)) dependence of the inclusive jet
production cross section in pp(macro) collisions at square
root of s = 1.8 TeV using 95 pb(-1) of data collected with
the D0 detector at the Fermilab Tevatron. The differential
cross section d(2)sigma/(dE(T)d eta) is presented up to eta
= 3, significantly extending previous measurements. The
results are in good overall agreement with next-to-leading
order predictions from QCD and indicate a preference for
certain parton distribution functions.},
Doi = {10.1103/physrevlett.86.1707},
Key = {fds308182}
}
@article{fds308056,
Author = {Abulencia, and A, and others},
Title = {Inclusive search for new physics with like-sign dilepton
events in $p \bar{p}$ collisions at $\sqrt{s}$ =
1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {22},
Pages = {221803},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.221803},
Abstract = {We describe a search for anomalous production of events with
two leptons (e or µ) of the same electric charge in
p[overline p] collisions at a center-of-mass energy of 1.96
TeV. Many extensions to the standard model predict the
production of two leptons of the same electric charge. This
search has a significant increase in sensitivity compared to
earlier searches. Using a data sample corresponding to 1
fb-1 of integrated luminosity recorded by the CDF II
detector, we observe no significant excess in an inclusive
selection (expect 33.2$\pm$4.7 events, observe 44) or in a
supersymmetry-optimized selection (expect 7.8$\pm$1.1
events, observe 13.)},
Doi = {10.1103/physrevlett.98.221803},
Key = {fds308056}
}
@article{fds307837,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
Title = {Inclusive search for same-sign dilepton signatures in pp
collisions at √s = 7 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2011},
Number = {10},
Pages = {1-47},
Publisher = {Springer Nature},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2011)107},
Abstract = {An inclusive search is presented for new physics in events
with two isolated leptons (e or μ) having the same electric
charge. The data are selected from events collected from pp
collisions at √s = 7 TeV by the ATLAS detector and
correspond to an integrated luminosity of 34 pb-1. The
spectra in dilepton invariant mass, missing transverse
momentum and jet multiplicity are presented and compared to
Standard Model predictions. In this event sample, no
evidence is found for contributions beyond those of the
Standard Model. Limits are set on the cross-section in a
fiducial region for new sources of same-sign high-mass
dilepton events in the ee, eμ and μμ channels. Four
models predicting same-sign dilepton signals are
constrained: two descriptions of Majorana neutrinos, a
cascade topology similar to supersymmetry or universal extra
dimensions, and fourth generation d-type quarks. Assuming a
new physics scale of 1 TeV, Majorana neutrinos produced by
an effective operator V with masses below 460 GeV are
excluded at 95% confidence level. A lower limit of 290 GeV
is set at 95% confidence level on the mass of fourth
generation d-type quarks. Copyright CERN.},
Doi = {10.1007/JHEP10(2011)107},
Key = {fds307837}
}
@article{fds307956,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart,
D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher,
A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi,
C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and da Costa, JG and Gunay-Unalan, Z and Haber, C and Hahn,
K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher,
F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko,
BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal,
AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone,
S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Griso,
SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts,
K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder,
N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Ramakrishnan, V and Ranjan, N and Redondo, I and Rekovic, V and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt,
MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider,
FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas,
J},
Title = {Inclusive search for squark and gluino production in pp[over
] collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {12},
Pages = {121801},
Year = {2009},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.102.121801},
Abstract = {We report on a search for inclusive production of squarks
and gluinos in pp[over ] collisions at sqrt[s]=1.96 TeV, in
events with large missing transverse energy and multiple
jets of hadrons in the final state. The study uses a CDF Run
II data sample corresponding to 2 fb(-1) of integrated
luminosity. The data are in good agreement with the standard
model predictions, giving no evidence for any squark or
gluino component. In an R-parity conserving minimal
supergravity scenario with A(0)=0, mu<0, and tanbeta=5, 95%
C.L. upper limits on the production cross sections in the
range between 0.1 and 1 pb are obtained, depending on the
squark and gluino masses considered. For gluino masses below
280 GeV/c(2), arbitrarily large squark masses are excluded
at the 95% C.L., while for mass degenerate gluinos and
squarks, masses below 392 GeV/c(2) are excluded at the 95%
C.L.},
Doi = {10.1103/physrevlett.102.121801},
Key = {fds307956}
}
@article{fds307912,
Author = {Aaltonen, and T, and others},
Title = {Inclusive Search for Standard Model Higgs Boson Production
in the WW Decay Channel using the CDF II
Detector},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {6},
Pages = {061803},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.061803},
Abstract = {http://arxiv.org/abs/1001.4468},
Doi = {10.1103/PhysRevLett.104.061803},
Key = {fds307912}
}
@booklet{Adams97,
Author = {M. R. Adams and M. Aderholz and S. Aid and P. L. Anthony and D. A. Averill and M. D. Baker and B. R. Baller and A.
Banerjee and A. A. Bhatti and U. Bratzler and H. M. Braun and T. J. Carroll and H. L. Clark and J. M. Conrad and R.
Davisson and I. Derado a},
Title = {Inclusive single-particle distributions and transverse
momenta of forward produced charged hadrons in mu p
scattering at 470 GeV},
Journal = {Zeitschrift Fur Physik C-particles And Fields},
Volume = {76},
Number = {3},
Pages = {441 -- 463},
Year = {1997},
Month = {November},
Key = {Adams97}
}
@article{fds308252,
Author = {Adams, MR and Aderholz, M and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dietrich, FS and Dougherty, W and Dreyer, T and Eckardt,
V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufmann, S and Kennedy, RD and Kinney, ER and Kobrak, HGE and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and Novak, J and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Röser, A and Ryan, JJ and Salgado, CW and Schellman, H and Schmitt, M and Schmitz, N and Schüler, KP and Seyerlein, J and Siegert, G and Skuja,
A and Snow, GA and Söldner-Rembold, S and Spentzouris, P and Stopa, P and Swanson, RA and Venkataramania, H and Wilhelm, M and Wilson, R and Wittek, W and Wolbers, SA and Zghiche, A and Zhao,
T},
Title = {Inclusive single-particle distributions and transverse
momenta of forward produced charged hadrons in μp
scattering at 470 GeV},
Journal = {Zeitschrift fur Physik C-Particles and Fields},
Volume = {76},
Number = {3},
Pages = {441-463},
Publisher = {Springer Nature},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1007/s002880050567},
Abstract = {Using data from the Fermilab fixed target experiment E665,
general properties of forward produced charged hadrons in
μp interactions at a primary muon energy of 470 GeV are
investigated. The normalized inclusive single-particle
distributions for Feynman-x D(xF) and for the transverse
momentum D(pt2, xF) are measured as a function of W and Q2.
The dependence of the average transverse momentum squared
〈pt2〉 on xF, W and Q2 is studied. The increasing
contribution from diffractive production as Q2 decreases
leads to a reduction of the average charged hadron
multiplicities at low (positive) xF and an enhancement at
large xF, for Q2 ≲ 10 GeV2. It also reduces 〈pt2〉 for
Q2 ≲ 5 GeV2 and 0.4 ≲ xF < 1.0. © Springer-Verlag
1997.},
Doi = {10.1007/s002880050567},
Key = {fds308252}
}
@article{fds346200,
Author = {Sinha, T and Karan, SC and Kotwal, A},
Title = {Increased urinary uric acid excretion: a finding in Indian
stone formers.},
Journal = {Urological research},
Volume = {38},
Number = {1},
Pages = {17-20},
Year = {2010},
Month = {February},
url = {http://dx.doi.org/10.1007/s00240-009-0236-y},
Abstract = {Many studies have been done to determine the risk factors
associated with urolithiasis so that preventive measures can
be undertaken to prevent stone formation. However the exact
aetiology of urinary stones still remains elusive. A
prospective control study of epidemiological factors that
influence urinary stone formation was done to determine the
aetiology of urinary stones. Patients with stone disease had
a significantly higher body mass index. 24-h urine excretion
of uric acid and phosphate was found to be significantly
higher in stone patients as compared to controls. The intake
of non-vegetarian food was significantly higher amongst
stone formers. Stone patients had a significantly higher
consumption of curd and cheese as compared to controls.
There was a significant correlation noted between stone
formation and a positive family and past history of stone
disease. The results indicate that obese patients,
especially those with a family history of stone disease,
should be counselled on weight loss. Individuals with a past
history of stone disease should be advised to reduce their
dietary intake of foods rich in uric acid (meat, liver and
beans).},
Doi = {10.1007/s00240-009-0236-y},
Key = {fds346200}
}
@article{fds346190,
Author = {Yadav, AK and Kotwal, A and Gupta, H and Kulkarni, A and Verma,
AK},
Title = {India without Poliomyelitis: Time to Make it a
Reality.},
Journal = {Indian journal of community medicine : official publication
of Indian Association of Preventive & Social
Medicine},
Volume = {37},
Number = {1},
Pages = {1-4},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.4103/0970-0218.94005},
Doi = {10.4103/0970-0218.94005},
Key = {fds346190}
}
@article{fds307540,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Indirect measurement of sin2θW (or MW) using μ+μ- pairs
from γ* /Z bosons produced in p p ̄ collisions at a
center-of-momentum energy of 1.96 TeV INDIRECT MEASUREMENT
of sin2θW (OR ... T. AALTONEN et al.},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072005},
Abstract = {Drell-Yan lepton pairs are produced in the process
pp̄→μ+μ- +X through an intermediate γ*/Zboson. The
forward-backward asymmetry in the polar-angle distribution
of the μ- as a function of the invariant mass of the μ+μ-
pair is used to obtain the effective leptonic determination
sin2θefflept of the electroweak-mixing parameter sin2θW,
from which the value of sin2θW is derived assuming the
standard model. The measurement sample, recorded by the
Collider Detector at Fermilab (CDF), corresponds to 9.2fb-1
of integrated luminosity from pp̄ collisions at a
center-of-momentum energy of 1.96 TeV, and is the full CDF
Run II data set. The value of sin2θefflept is found to be
0.2315±0. 0010, where statistical and systematic
uncertainties are combined in quadrature. When interpreted
within the context of the standard model using the on-shell
renormalization scheme, where sin2θW=1-MW2/MZ2, the
measurement yields sin2θW=0.2233±0.0009, or equivalently a
W-boson mass of 80.365±0.047GeV/c2. The value of the
W-boson mass is in agreement with previous determinations in
electron-positron collisions and at the Tevatron collider.
© 2014 American Physical Society.},
Doi = {10.1103/PhysRevD.89.072005},
Key = {fds307540}
}
@article{fds310399,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Indirect measurement of sin2θw (MW)
using e+e- pairs in the Z-boson region
with p̄p collisions at a center-of-momentum energy of 1.96
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.072002},
Abstract = {Drell-Yan lepton pairs are produced in the process p̄p→e
+e-+X through an intermediate γ*/Z boson. The lepton
angular distributions are used to provide information on the
electroweak-mixing parameter sin2θw via its observable
effective-leptonic sin2θw, or sinâ¡2θefflept. A new
method to infer sin 2θw or, equivalently, the W-boson mass
MW in the on-shell scheme, is developed and tested using a
previous CDF Run II measurement of angular distributions
from electron pairs in a sample corresponding to 2.1 fb-1 of
integrated luminosity from p̄p collisions at a
center-of-momentum energy of 1.96 TeV. The value of
sinâ¡2θefflept is found to be 0.2328±0.0011. Within a
specified context of the standard model, this results in sin
2θw=0.2246±0.0011, which corresponds to a W-boson mass of
80.297±0.055 GeV/c2, in agreement with previous
determinations in electron-position collisions and at the
Tevatron collider. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.072002},
Key = {fds310399}
}
@article{fds346194,
Author = {Minhas, S and Kotwal, A and Singh, M},
Title = {Infection Control in Health Care Facilities.},
Journal = {Medical journal, Armed Forces India},
Volume = {67},
Number = {1},
Pages = {7-8},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1016/s0377-1237(11)80003-1},
Doi = {10.1016/s0377-1237(11)80003-1},
Key = {fds346194}
}
@article{fds346182,
Author = {Ayub, A and Goyal, A and Kotwal, A and Kulkarni, A and Kotwal, A and Mahen,
A},
Title = {Infection control practices in health care: Teaching and
learning requirements of medical undergraduates.},
Journal = {Medical journal, Armed Forces India},
Volume = {69},
Number = {2},
Pages = {107-112},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.07.021},
Abstract = {<h4>Background</h4>Compliance and implementation of
infection control guidelines have been recognized as
efficient means to prevent and control hospital acquired
infections.<h4>Objectives</h4>To evaluate knowledge and
practices about infection control guidelines amongst medical
students and to explore their education needs as perceived
by them and faculty.<h4>Methods</h4>A total of 160 final
year students and 100 faculty members of one of the top
medical colleges in India were selected by simple random
sampling in each group as per sample size of 143 students
(alpha 0.05, error 7%, prevalence 60%) and 99 (error 7.5%)
faculty. Data collected by pilot-tested, unlinked, anonymous
questionnaire.<h4>Results</h4>Amongst students, knowledge
(77.50%; 95% CI, 70.24-83.72) was mixed with misconceptions.
Only 31.25% always followed hand hygiene procedure; 50%
recapped needles; disposal of hazardous material into
designated containers always was low (sharps 20%,
contaminated items 25%). Despite experiencing needle stick
injury (6.25%) and splashes (40%), less than 30% reported
these as 44% were unaware of reporting procedure. The
discord between the perceptions of faculty regarding
students and students' own perceptions was clearly evident
(all Kappa values less than 0.50). Students and faculty
agreed on workshops (58.13% and 58%) and reinforcement by
colleagues (51% and 54%) but not on on-job training (51% and
34%) and part of curriculum (48% and 40%) for
teaching-learning infection control.<h4>Conclusion</h4>Tackling
disconnect between students and faculty perceptions and
empowering students with knowledge and skills in infection
control is important. Approach needs to be researched and
formulated as current methods seem to be
inadequate.},
Doi = {10.1016/j.mjafi.2012.07.021},
Key = {fds346182}
}
@article{fds341507,
Author = {Chekanov, SV and Beydler, M and Kotwal, AV and Gray, L and Sen, S and Tran,
NV and Yu, SS and Zuzelski, J},
Title = {Initial performance studies of a general-purpose detector
for multi-TeV physics at a 100 TeV pp collider},
Journal = {Journal of Instrumentation},
Volume = {12},
Number = {6},
Year = {2017},
Month = {June},
url = {http://dx.doi.org/10.1088/1748-0221/12/06/P06009},
Abstract = {This paper describes simulations of detector response to
multi-TeV particles and jets at the Future Circular Collider
(FCC-hh) or Super proton-proton Collider (SppC) which aim to
collide proton beams with a centre-of-mass energy of 100
TeV. The unprecedented energy regime of these future
experiments imposes new requirements on detector
technologies which can be studied using the detailed GEANT4
simulations presented in this paper. The initial performance
of a detector designed for physics studies at the FCC-hh or
SppC experiments is described with an emphasis on
measurements of single particles up to 33 TeV in transverse
momentum. The reconstruction of hadronic jets has also been
studied in the transverse momentum range from 50 GeV to 26
TeV. The granularity requirements for calorimetry are
investigated using the two-particle spatial resolution
achieved for hadron showers.},
Doi = {10.1088/1748-0221/12/06/P06009},
Key = {fds341507}
}
@article{fds346218,
Author = {Kotwal, A and Priya, R and Thakur, R and Gupta, V and Kotwal, J and Seth,
T},
Title = {Injection practices in a metropolis of North India:
perceptions, determinants and issues of safety.},
Journal = {Indian journal of medical sciences},
Volume = {58},
Number = {8},
Pages = {334-344},
Year = {2004},
Month = {August},
Abstract = {<h4>Background</h4>At least 50 percent of the injections
administered each year are unsafe, more particularly in
developing countries, posing serious health risks. An
initial assessment to describe injection practices; their
determinants and adverse effects can prevent
injection-associated transmission of blood borne pathogens
by reducing injection frequency and adoption of safe
injection practices.<h4>Aims</h4>To assess the injection
practices in a large metropolitan city encompassing varied
socio-cultural scenarios. STUDY SETTING AND DESIGN: Field
based cross sectional survey covering urban non-slum, slum
and peri-urban areas of a large metropolitan
city.<h4>Methods and material</h4>Injection prescribers,
providers and community members selected by random sampling
from the study areas. Pre tested questionnaires assessed
knowledge and perceptions of study subjects towards
injections and their possible complications. Observation of
the process of injection and prescription audit also carried
out.<h4>Statistical analysis</h4>MS Access for database and
SPSS ver 11 for analysis. Point estimates, 95% confidence
intervals, Chi Square, t test, one-way ANOVA.<h4>Results</h4>The
per capita injection rate was 5.1 per year and ratio of
therapeutic to immunization injections was 4.4:1. Only
22.5%of injections were administered with a sterile syringe
and needle. The level of knowledge about HIV and HBV
transmission by unsafe injections was satisfactory amongst
prescribers and community, but inadequate amongst providers.
HCV was known to a very few in all the groups. The annual
incidence of needle stick injuries among providers was quite
high.<h4>Conclusion</h4>A locally relevant safe injection
policy based on multi disciplinary approach is required to
reduce number of injections, unsafe injections and their
attendant complications.},
Key = {fds346218}
}
@article{fds346199,
Author = {Kotwal, A},
Title = {Injections need for reduction, safety and
appropriateness.},
Journal = {Indian pediatrics},
Volume = {47},
Number = {5},
Pages = {399-400},
Year = {2010},
Month = {May},
url = {http://dx.doi.org/10.1007/s13312-010-0071-9},
Doi = {10.1007/s13312-010-0071-9},
Key = {fds346199}
}
@article{fds346215,
Author = {Kotwal, A},
Title = {Innovation, diffusion and safety of a medical technology: a
review of the literature on injection practices.},
Journal = {Social science & medicine (1982)},
Volume = {60},
Number = {5},
Pages = {1133-1147},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1016/j.socscimed.2004.06.044},
Abstract = {The rapid uptake of the hypodermic syringe as a medical
technology by physicians in Europe and America since its
introduction in the middle of the 19th century has led to a
level of medical and public acceptance seldom reached by
other therapeutic techniques. Presently, the developed world
has clear guidelines regarding injection use and safety; in
contrast, developing countries are facing the brunt of risks
associated with the use of this technology, which was
introduced into their societies during the early 20th
century. There is now a popular demand for injections, and
an alarming number of unnecessary and unsafe injections are
being administered. The problem of unsafe injections is not
restricted to curative injections, but includes
immunizations too. The association of unsafe injections and
infection transmission is quite clear, and there is an
urgent need to reduce the number of required injections and
make them safe. An understanding of the determinants of
current injection practices in the socio-cultural-economic
context is necessary in order to plan relevant and effective
interventions.},
Doi = {10.1016/j.socscimed.2004.06.044},
Key = {fds346215}
}
@article{fds346181,
Author = {Kotwal, A},
Title = {Innovations in teaching/learning methods for medical
students: research with mentoring.},
Journal = {Indian journal of public health},
Volume = {57},
Number = {3},
Pages = {144-146},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.4103/0019-557x.119822},
Abstract = {In this era of evidence-based medicine, innovative teaching
learning methods coupled with appropriate mentoring are
required to make the undergraduate medical students
interested in the speciality of Community Medicine. Teaching
research methodology to medical students by a hands-on
approach along with mentoring by involving them in small,
feasible, sustainable, and replicable studies on a topic of
interest clearly showed renewed interest among students
toward the subject.},
Doi = {10.4103/0019-557x.119822},
Key = {fds346181}
}
@article{fds308157,
Author = {Hays, C and Huang, Y and Kotwal, AV and Gerberich, HK and Menzemer, S and Rinnert, K and Lecci, C and Herndon, M and Snider,
FD},
Title = {Inside-out tracking at CDF},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {538},
Number = {1-3},
Pages = {249-254},
Publisher = {Elsevier BV},
Year = {2005},
Month = {February},
url = {http://dx.doi.org/10.1016/j.nima.2004.08.104},
Abstract = {The Central Outer Tracker (COT) at the Collider Detector at
Fermilab (CDF) is used to reconstruct charged particles in
the central rapidity region. The silicon tracker is used to
improve the central track measurement and to reconstruct
charged particles in the forward rapidity region. We
describe the inside-out tracking algorithm, which improves
the track measurement in the intermediate rapidity region by
attaching COT hits to reconstructed silicon tracks. © 2004
Elsevier B.V. All rights reserved.},
Doi = {10.1016/j.nima.2004.08.104},
Key = {fds308157}
}
@article{fds30153,
Author = {Christopher Hays and Yimei Huang and Ashutosh V. Kotwal and Heather
K. Gerberich and Stephanie Menzemer and Kurt Rinnert and Claudia
Lecci, Matthew Herndon and Frederick D. Snider},
Title = {Inside-out tracking at CDF},
Journal = {Nuclear Instruments and Methods in Physics Research Section
A},
Year = {2004},
Month = {September},
Key = {fds30153}
}
@article{fds374212,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Castillo, FL and Costanza, F and Delmastro, M and Di
Ciaccio, L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo
Martinez, N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Li, T and Marchiori, G and Nakkalil, K and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wamorkar, T and Wang, R and Zhang, J and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost,
M},
Title = {Integrated and differential fiducial cross-section
measurements for the vector boson fusion production of the
Higgs boson in the H →WW∗→eνμν decay channel at 13
TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {108},
Number = {7},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.108.072003},
Abstract = {The vector-boson production cross section for the Higgs
boson decay in the Formula Presented channel is measured as
a function of kinematic observables sensitive to the Higgs
boson production and decay properties as well as integrated
in a fiducial phase space. The analysis is performed using
the proton-proton collision data collected by the ATLAS
detector in Run 2 of the LHC at Formula Presented
center-of-mass energy, corresponding to an integrated
luminosity of Formula Presented. The different flavor final
state is studied by selecting an electron and a muon
originating from a pair of Formula Presented bosons and
compatible with the Higgs boson decay. The data are
corrected for the effects of detector inefficiency and
resolution, and the measurements are compared with different
state-of-the-art theoretical predictions. The differential
cross sections are used to constrain anomalous interactions
described by dimension-six operators in an effective field
theory.},
Doi = {10.1103/PhysRevD.108.072003},
Key = {fds374212}
}
@article{fds307848,
Author = {Aaltonen, and T, and al, E},
Title = {Invariant Mass Distribution of Jet Pairs Produced in
Association with a ${W}$ Boson in $p\overline{p}$ Collisions
at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {17},
Pages = {171801},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.171801},
Abstract = {We report a study of the invariant mass distribution of jet
pairs produced in association with a W boson using data
collected with the CDF detector which correspond to an
integrated luminosity of 4.3 fb(-1). The observed
distribution has an excess in the 120-160 GeV/c(2) mass
range which is not described by current theoretical
predictions within the statistical and systematic
uncertainties. In this Letter, we report studies of the
properties of this excess.},
Doi = {10.1103/PhysRevLett.106.171801},
Key = {fds307848}
}
@article{fds307536,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Invariant-mass distribution of jet pairs produced in
association with a W boson in p p ̄ collisions at s
=1.96TeV using the full CDF Run II data set invariant-mass
distribution of ⋯ T. Aaltonen et al.},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {9},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.89.092001},
Abstract = {We report on a study of the dijet invariant-mass
distribution in events with one identified lepton, a
significant imbalance in the total event transverse
momentum, and two jets. This distribution is sensitive to
the possible production of a new particle in association
with a W boson, where the boson decays leptonically. We use
the full data set of proton-antiproton collisions at 1.96
TeV center-of-mass energy collected by the Collider Detector
at the Fermilab Tevatron, corresponding to an integrated
luminosity of 8.9fb-1. The data are found to be consistent
with standard model expectations, and a 95% confidence level
upper limit is set on the production cross section of a W
boson in association with a new particle decaying into two
jets. © 2014 American Physical Society.},
Doi = {10.1103/PhysRevD.89.092001},
Key = {fds307536}
}
@article{fds346196,
Author = {Kotwal, A},
Title = {Iodine deficiency disorders: a health policy and planning
perspective.},
Journal = {Indian journal of public health},
Volume = {54},
Number = {4},
Pages = {175-178},
Year = {2010},
Month = {October},
url = {http://dx.doi.org/10.4103/0019-557x.77255},
Doi = {10.4103/0019-557x.77255},
Key = {fds346196}
}
@article{fds308203,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buescher,
V and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum,
Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev,
SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and di Loreto, G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison,
J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
T and Feher, S and Fein, D and Ferbel, T},
Title = {Isolated photon cross section in p p̄ collisions at √s =
1.8 TeV},
Journal = {Physical Review Letters},
Volume = {84},
Number = {13},
Pages = {2786-2791},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.2786},
Abstract = {We report a new measurement of the cross section for the
production of isolated photons with transverse energies (E
Tγ) above 10 GeV and pseudorapidities |η| < 2.5 in p̄
collisions at √s = 1.8 TeV. The results are based on a
data sample of 107.6 pb -1 recorded during 1992-1995 with
the D0 detector at the Fermilab Tevatron collider. The
background, predominantly from jets which fragment to
neutral mesons, was estimated using the longitudinal shower
shape of photon candidates in the calorimeter. The measured
cross section is in good agreement with the next-to-leading
order QCD calculation for E Tγ ≳ 36 GeV. © 2000 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.84.2786},
Key = {fds308203}
}
@article{fds310309,
Author = {Atlas Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes,
GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burghgrave,
B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey,
P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH},
Title = {Jet energy measurement and its systematic uncertainty in
proton-proton collisions at [Formula: see text] TeV with
the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Pages = {17},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3190-y},
Abstract = {The jet energy scale (JES) and its systematic uncertainty
are determined for jets measured with the ATLAS detector
using proton-proton collision data with a centre-of-mass
energy of [Formula: see text] TeV corresponding to an
integrated luminosity of [Formula: see text][Formula: see
text]. Jets are reconstructed from energy deposits forming
topological clusters of calorimeter cells using the
anti-[Formula: see text] algorithm with distance parameters
[Formula: see text] or [Formula: see text], and are
calibrated using MC simulations. A residual JES correction
is applied to account for differences between data and MC
simulations. This correction and its systematic uncertainty
are estimated using a combination of in situ techniques
exploiting the transverse momentum balance between a jet and
a reference object such as a photon or a [Formula: see text]
boson, for [Formula: see text] and pseudorapidities
[Formula: see text]. The effect of multiple proton-proton
interactions is corrected for, and an uncertainty is
evaluated using in situ techniques. The smallest JES
uncertainty of less than 1 % is found in the central
calorimeter region ([Formula: see text]) for jets with
[Formula: see text]. For central jets at lower [Formula: see
text], the uncertainty is about 3 %. A consistent JES
estimate is found using measurements of the calorimeter
response of single hadrons in proton-proton collisions and
test-beam data, which also provide the estimate for
[Formula: see text] TeV. The calibration of forward jets is
derived from dijet [Formula: see text] balance measurements.
The resulting uncertainty reaches its largest value of 6 %
for low-[Formula: see text] jets at [Formula: see text].
Additional JES uncertainties due to specific event
topologies, such as close-by jets or selections of event
samples with an enhanced content of jets originating from
light quarks or gluons, are also discussed. The magnitude of
these uncertainties depends on the event sample used in a
given physics analysis, but typically amounts to
0.5-3 %.},
Doi = {10.1140/epjc/s10052-014-3190-y},
Key = {fds310309}
}
@article{fds307621,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A},
Title = {Jet energy measurement with the ATLAS detector in
proton-proton collisions at √s =7 TeV},
Journal = {European Physical Journal C},
Volume = {73},
Number = {3},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2304-2},
Abstract = {The jet energy scale and its systematic uncertainty are
determined for jets measured with the ATLAS detector at the
LHC in proton-proton collision data at a centre-of-mass
energy of √ s = 7 TeV corresponding to an integrated
luminosity of 38 pb-1. Jets are reconstructed with the
anti-kt algorithm with distance parameters R = 0.4 or R =
0.6. Jet energy and angle corrections are determined from
Monte Carlo simulations to calibrate jets with transverse
momenta pT ≥ 20 GeV and pseudorapidities |η| < 4.5. The
jet energy systematic uncertainty is estimated using the
single isolated hadron response measured in situ and in
test-beams, exploiting the transverse momentum balance
between central and forward jets in events with dijet
topologies and studying systematic variations in Monte Carlo
simulations. The jet energy uncertainty is less than 2.5 %
in the central calorimeter region (|η| < 0.8) for jets with
60 ≤ pT < 800 GeV, and is maximally 14 % for pT ≤ 30 GeV
in the most forward region 3.2 ≤ |η| < 4.5. The jet
energy is validated for jet transverse momenta up to 1 TeV
to the level of a few percent using several in situ
techniques by comparing a well-known reference such as the
recoiling photon pT, the sum of the transverse momenta of
tracks associated to the jet, or a system of low-pT jets
recoiling against a high-pT jet. More sophisticated jet
calibration schemes are presented based on calorimeter cell
energy density weighting or hadronic properties of jets,
aiming for an improved jet energy resolution and a reduced
flavour dependence of the jet response. The systematic
uncertainty of the jet energy determined from a combination
of in situ techniques is consistent with the one derived
from single hadron response measurements over a wide
kinematic range. The nominal corrections and uncertainties
are derived for isolated jets in an inclusive sample of
high-pT jets. Special cases such as event topologies with
close-by jets, or selections of samples with an enhanced
content of jets originating from light quarks, heavy quarks
or gluons are also discussed and the corresponding
uncertainties are determined.},
Doi = {10.1140/epjc/s10052-013-2304-2},
Key = {fds307621}
}
@article{fds307615,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo
Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG},
Title = {Jet energy resolution in proton-proton collisions at
[Formula: see text] recorded in 2010 with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {3},
Pages = {2306},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2306-0},
Abstract = {The measurement of the jet energy resolution is presented
using data recorded with the ATLAS detector in proton-proton
collisions at [Formula: see text]. The sample corresponds to
an integrated luminosity of 35 pb<sup>-1</sup>. Jets are
reconstructed from energy deposits measured by the
calorimeters and calibrated using different jet calibration
schemes. The jet energy resolution is measured with two
different in situ methods which are found to be in agreement
within uncertainties. The total uncertainties on these
measurements range from 20 % to 10 % for jets within
|<i>y</i>|<2.8 and with transverse momenta increasing
from 30 GeV to 500 GeV. Overall, the Monte Carlo
simulation of the jet energy resolution agrees with the data
within 10 %.},
Doi = {10.1140/epjc/s10052-013-2306-0},
Key = {fds307615}
}
@article{fds358460,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Jet energy scale and resolution measured in proton–proton
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {8},
Year = {2021},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09402-3},
Abstract = {Jet energy scale and resolution measurements with their
associated uncertainties are reported for jets using
36–81 fb- 1 of proton–proton collision data with a
centre-of-mass energy of s=13 TeV collected by the ATLAS
detector at the LHC. Jets are reconstructed using two
different input types: topo-clusters formed from energy
deposits in calorimeter cells, as well as an algorithmic
combination of charged-particle tracks with those
topo-clusters, referred to as the ATLAS particle-flow
reconstruction method. The anti-kt jet algorithm with radius
parameter R= 0.4 is the primary jet definition used for both
jet types. This result presents new jet energy scale and
resolution measurements in the high pile-up conditions of
late LHC Run 2 as well as a full calibration of
particle-flow jets in ATLAS. Jets are initially calibrated
using a sequence of simulation-based corrections. Next,
several in situ techniques are employed to correct for
differences between data and simulation and to measure the
resolution of jets. The systematic uncertainties in the jet
energy scale for central jets (| η| < 1.2) vary from 1% for
a wide range of high-pT jets (250<pT<2000GeV), to 5% at very
low pT (20GeV) and 3.5% at very high pT (>2.5TeV). The
relative jet energy resolution is measured and ranges from
(24 ± 1.5)% at 20 GeV to (6 ± 0.5)% at
300 GeV.},
Doi = {10.1140/epjc/s10052-021-09402-3},
Key = {fds358460}
}
@article{fds356729,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Jet energy scale measurements and their systematic
uncertainties in proton-proton collisions at s =13 TeV with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {96},
Number = {7},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.96.072002},
Abstract = {Jet energy scale measurements and their systematic
uncertainties are reported for jets measured with the ATLAS
detector using proton-proton collision data with a
center-of-mass energy of s=13 TeV, corresponding to an
integrated luminosity of 3.2 fb-1 collected during 2015 at
the LHC. Jets are reconstructed from energy deposits forming
topological clusters of calorimeter cells, using the anti-kt
algorithm with radius parameter R=0.4. Jets are calibrated
with a series of simulation-based corrections and in situ
techniques. In situ techniques exploit the transverse
momentum balance between a jet and a reference object such
as a photon, Z boson, or multijet system for jets with
20<pT<2000 GeV and pseudorapidities of |η|<4.5, using both
data and simulation. An uncertainty in the jet energy scale
of less than 1% is found in the central calorimeter region
(|η|<1.2) for jets with 100<pT<500 GeV. An uncertainty of
about 4.5% is found for low-pT jets with pT=20 GeV in the
central region, dominated by uncertainties in the
corrections for multiple proton-proton interactions. The
calibration of forward jets (|η|>0.8) is derived from dijet
pT balance measurements. For jets of pT=80 GeV, the
additional uncertainty for the forward jet calibration
reaches its largest value of about 2% in the range |η|>3.5
and in a narrow slice of 2.2<|η|<2.4.},
Doi = {10.1103/PhysRevD.96.072002},
Key = {fds356729}
}
@article{fds307776,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Jet mass and substructure of inclusive jets in √s = 7TeV
pp collisions with the ATLAS experiment},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {5},
Publisher = {Springer Nature},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP05(2012)128},
Abstract = {Recent studies have highlighted the potential of jet
substructure techniques to identify the hadronic decays of
boosted heavy particles. These studies all rely upon the
assumption that the internal substructure of jets generated
by QCD radiation is well understood. In this article, this
assumption is tested on an inclusive sample of jets recorded
with the ATLAS detector in 2010, which corresponds to 35 pb
-1 of pp collisions delivered by the LHC at Rs =
7TeV.},
Doi = {10.1007/JHEP05(2012)128},
Key = {fds307776}
}
@article{fds347508,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos,
SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul,
A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard,
DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair,
RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger,
AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr,
JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret,
MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini,
M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney,
RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carvalho,
J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
Title = {Jet reconstruction and performance using particle flow with
the ATLAS Detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {7},
Pages = {466},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5031-2},
Abstract = {This paper describes the implementation and performance of a
particle flow algorithm applied to 20.2 fb[Formula: see
text] of ATLAS data from 8 TeV proton-proton collisions in
Run 1 of the LHC. The algorithm removes calorimeter energy
deposits due to charged hadrons from consideration during
jet reconstruction, instead using measurements of their
momenta from the inner tracker. This improves the accuracy
of the charged-hadron measurement, while retaining the
calorimeter measurements of neutral-particle energies. The
paper places emphasis on how this is achieved, while
minimising double-counting of charged-hadron signals between
the inner tracker and calorimeter. The performance of
particle flow jets, formed from the ensemble of signals from
the calorimeter and the inner tracker, is compared to that
of jets reconstructed from calorimeter energy deposits
alone, demonstrating improvements in resolution and pile-up
stability.},
Doi = {10.1140/epjc/s10052-017-5031-2},
Key = {fds347508}
}
@article{fds349662,
Author = {Yeh, CH and Chekanov, SV and Kotwal, AV and Proudfoot, J and Sen, S and Tran, NV and Yu, SS},
Title = {Jet substructure variables with the SiFCC detector at 100
TeV},
Journal = {Proceedings of Science},
Volume = {340},
Year = {2019},
Month = {January},
Abstract = {Future experiments beyond the LHC era will measure
high-momentum bosons (W, Z, H) and top quarks with strongly
collimated decay products that form hadronic jets. This
paper describes the studies of the performance of jet
substructure variables using the Geant4 simulation of a
detector designed for high energy pp collisions at a 100 TeV
collider. The two-prong jets from Z′ → WW and
three-prong jets from Z′ → tt&tild; are compared with
the background from light quark jets, assuming Z′ masses
in the range 5 - 40 TeV. Our results indicate that the
performance of jetsubstructure reconstruction improves with
reducing transverse cell sizes of a hadronic calorimeter
from Δη × Δφ = 0:087×0:087 to 0:022×0:022 in most
cases.},
Key = {fds349662}
}
@article{fds364960,
Author = {Bonilla, J and Chachamis, G and Dillon, BM and Chekanov, SV and Erbacher, R and Gouskos, L and Hinzmann, A and Höche, S and Huffman,
BT and Kotwal, AV and Kar, D and Kogler, R and Lange, C and LeBlanc, M and Lemmon, R and McLean, C and Nachman, B and Neubauer, MS and Plehn, T and Rappoccio, S and Roy, D and Roloff, J and Stark, G and Tran, N and Vos, M and Yeh, C-H and Yu, S-S},
Title = {Jets and Jet Substructure at Future Colliders},
Journal = {Frontiers in Physics},
Volume = {10},
Publisher = {Frontiers Media SA},
Year = {2022},
Month = {June},
url = {http://dx.doi.org/10.3389/fphy.2022.897719},
Abstract = {<jats:p>Even though jet substructure was not an original
design consideration for the Large Hadron Collider (LHC)
experiments, it has emerged as an essential tool for the
current physics program. We examine the role of jet
substructure on the motivation for and design of future
energy Frontier colliders. In particular, we discuss the
need for a vibrant theory and experimental research and
development program to extend jet substructure physics into
the new regimes probed by future colliders. Jet substructure
has organically evolved with a close connection between
theorists and experimentalists and has catalyzed exciting
innovations in both communities. We expect such developments
will play an important role in the future energy Frontier
physics program.</jats:p>},
Doi = {10.3389/fphy.2022.897719},
Key = {fds364960}
}
@article{fds307745,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
G and Arutinov, D},
Title = {Ks0 and Λ production in pp interactions at √s=0.9 and 7
TeV measured with the ATLAS detector at the
LHC},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012001},
Abstract = {The production of KS0 and Λ hadrons is studied in pp
collision data at √s=0.9 and 7 TeV collected with the
ATLAS detector at the LHC using a minimum-bias trigger. The
observed distributions of transverse momentum, rapidity, and
multiplicity are corrected to hadron level in a
model-independent way within well-defined phase-space
regions. The distribution of the production ratio of Λ̄ to
Λ baryons is also measured. The results are compared with
various Monte Carlo simulation models. Although most of
these models agree with data to within 15% in the KS0
distributions, substantial disagreements are found in the Λ
distributions of transverse momentum. © 2012
CERN.},
Doi = {10.1103/PhysRevD.85.012001},
Key = {fds307745}
}
@article{fds347520,
Author = {Kotwal, A},
Title = {Letter to the Editor.},
Journal = {Medical journal, Armed Forces India},
Volume = {72},
Number = {1},
Pages = {95-96},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1016/j.mjafi.2015.10.003},
Doi = {10.1016/j.mjafi.2015.10.003},
Key = {fds347520}
}
@article{fds310387,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau,
M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli,
F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura,
AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {Light-quark and gluon jet discrimination in [Formula: see
text] collisions at [Formula: see text] with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {8},
Pages = {3023},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3023-z},
Abstract = {A likelihood-based discriminant for the identification of
quark- and gluon-initiated jets is built and validated using
4.7 fb[Formula: see text] of proton-proton collision data
at [Formula: see text] [Formula: see text] collected with
the ATLAS detector at the LHC. Data samples with enriched
quark or gluon content are used in the construction and
validation of templates of jet properties that are the input
to the likelihood-based discriminant. The discriminating
power of the jet tagger is established in both data and
Monte Carlo samples within a systematic uncertainty of
[Formula: see text] 10-20 %. In data, light-quark jets can
be tagged with an efficiency of [Formula: see text] while
achieving a gluon-jet mis-tag rate of [Formula: see text] in
a [Formula: see text] range between [Formula: see text] and
[Formula: see text] for jets in the acceptance of the
tracker. The rejection of gluon-jets found in the data is
significantly below what is attainable using a Pythia 6
Monte Carlo simulation, where gluon-jet mis-tag rates of
10 % can be reached for a 50 % selection efficiency of
light-quark jets using the same jet properties.},
Doi = {10.1140/epjc/s10052-014-3023-z},
Key = {fds310387}
}
@article{fds307841,
Author = {Aaltonen, and T, and al, E},
Title = {Limits on Anomalous Trilinear Gauge Couplings in ${Z}\gamma$
Events from $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {5},
Pages = {051802},
Publisher = {American Physical Society},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.051802},
Abstract = {Using Zγ candidate events collected by the CDF detector at
the Tevatron Collider, we search for potential anomalous
(non-standard-model) couplings between the Z boson and the
photon. Zγ couplings vanish at tree level and are heavily
suppressed at higher orders; hence any evidence of couplings
indicates new physics. Measurements are performed using data
corresponding to an integrated luminosity of 4.9 fb(-1)
in the Z→νν¯ decay channel and 5.1 fb(-1) in the
Z→l(+)l(-) (l=μ, e) decay channels. The combination of
these measurements provides the most stringent limits to
date on Zγ trilinear gauge couplings. Using an energy scale
of Λ=1.5 TeV to allow for a direct comparison with
previous measurements, we find limits on the CP-conserving
parameters that describe Zγ couplings to be
|h(3)(γ,Z)|<0.022 and |h(4)(γ,Z)|<0.0009. These results
are consistent with standard model predictions.},
Doi = {10.1103/PhysRevLett.107.051802},
Key = {fds307841}
}
@article{fds308064,
Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Behari,
S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak,
M},
Title = {Limits on anomalous triple gauge couplings in pp̄
collisions at s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {76},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.76.111103},
Abstract = {We present a search for anomalous triple gauge couplings
(ATGC) in WW and WZ boson production. The boson pairs are
produced in pp̄ collisions at s=1.96TeV, and the data
sample corresponds to 350pb-1 of integrated luminosity
collected with the CDF II detector at the Fermilab Tevatron.
In this search one W decays to leptons, and the other boson
(W or Z) decays hadronically. Combining with a previously
published CDF measurement of Wγ boson production yields
ATGC limits of -0.18<λ<0.17 and -0.46<Δκ<0.39 at the 95%
confidence level, using a cutoff scale Λ=1.5TeV. © 2007
The American Physical Society.},
Doi = {10.1103/PhysRevD.76.111103},
Key = {fds308064}
}
@booklet{Abbott98d,
Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
Alves and N. Amos and E. W. Anderson and R. Astur and M. M.
Baarmand and L. Babukhadia and A. Baden and V. Balamurali and J. Balderston},
Title = {Limits on anomalous WW gamma and WWZ couplings},
Journal = {Physical Review D},
Volume = {5803},
Number = {3},
Year = {1998},
Month = {August},
Key = {Abbott98d}
}
@article{fds308201,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Brass, A and Buchholz, D and Buescher,
V and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum,
Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev,
SV and Chen, LP and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper,
WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
D},
Title = {Limits on anomalous WWγ and WWZ couplings from WW/WZ→e
vjj production},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {62},
Number = {5},
Pages = {1-18},
Year = {2000},
Month = {September},
Abstract = {Limits on anomalous WWγ and WWZ couplings are presented
from a study of WW/WZ→e vjj events produced in pp̄
collisions at √s=1.8 TeV. Results from the analysis of
data collected using the DØ detector during the 1993-1995
Tevatron collider run at Fermilab are combined with those of
an earlier study from the 1992-1993 run. A fit to the
transverse momentum spectrum of the W boson yields direct
limits on anomalous WWγ and WWZ couplings. With the
assumption that the WWγ and WWZ couplings are equal, we
obtain -0.34<λ<0.36 (with Δκ=0) and -0.43<Δκ<0.59 (with
λ=0) at the 95% confidence level for a form-factor scale
Λ=2.0 TeV. ©2000 The American Physical
Society.},
Key = {fds308201}
}
@booklet{Abachi97d,
Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Álvarez, G and Alves,
GA and Amidi, E and Amos, N and Anderson, EW and Aronson, SH and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Bendich, J and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Bischoff, A and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt,
A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty,
D and Chang, S-M and Chekulaev, SV and Chen, L-P and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and De,
K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard,
J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahey, S and Fahland, T and Fatyga, M and Fatyga, MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC and Franzini, P and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Geld, TL and Genik II and RJ and Genser, K and Gerber, CE and Gibbard, B and Glebov, V and Glenn, S and Gobbi, B and Goforth, M and Goldschmidt, A and Gómez, B and Gomez, G and Goncharov,
PI and González Solís and JL and Gordon, H and Goss, LT and Goussiou, A and Graf, N and Grannis, PD and Green, DR and Green, J and Greenlee, H and Griffin, G and Grim, G and Grossman, N and Grudberg, P and Grünendahl,
S and Guglielmo, G and Guida, JA and Guida, JM and Guryn, W and Gurzhiev,
SN and Gutierrez, P and Gutnikov, YE and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hansen, S and Hauptman, JM and Hedin, D and Heinson, AP and Heintz, U and Hernández-Montoya, R and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hsieh, F and Hu, T and Hu, T and Huehn, T and Ito, AS and James, E and Jaques, J and Jerger, SA and Jiang, JZ-Y and Joffe-Minor, T and Johns, K and Johnson, M and Jonckheere, A and Jones,
M and Jöstlein, H and Jun, SY and Jung, CK and Kahn, S and Kalbfleisch, G and Kang, JS and Kehoe, R and Kelly, ML and Kerth, L and Kim, CL and Kim, SK and Klatchko, A and Klima, B and Klochkov, BI and Klopfenstein, C and Klyukhin, VI and Kochetkov, VI and Kohli, JM and Koltick, D and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kourlas, J and Kozelov, AV and Kozlovski, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kunori, S and Lami, S and Lan, H and Landsberg, G and Lauer, B and Lebrat, J-F and Leflat, A and Li, H and Li, J and Li, YK and Li-Demarteau, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Liu, Q and Liu, YC and Lobkowicz, F and Loken, SC and Lökös, S and Lueking, L and Lyon, AL and Maciel, AKA and Madaras, RJ and Madden, R and Magaña-Mendoza, L and Mani, S and Mao,
HS and Markeloff, R and Markosky, L and Marshall, T and Martin, MI and May,
B and Mayorov, AA and McCarthy, R and McDonald, J and McKibben, T and McKinley, J and McMahon, T and Melanson, HL and Merritt, KW and Miettinen, H and Mincer, A and de Miranda, JM and Mishra, CS and Mokhov,
N and Mondal, NK and Montgomery, HE and Mooney, P and da Motta, H and Mudan, M and Murphy, C and Nang, F and Narain, M and Narasimham, VS and Narayanan, A and Neal, HA and Negret, JP and Nemethy, P and Nes̆ić, D and Nicola, M and Norman, D and Oesch, L and Oguri, V and Oltman, E and Oshima,
N and Owen, D and Padley, P and Pang, M and Para, A and Park, YM and Partridge, R and Parua, N and Paterno, M and Perkins, J and Peters, M and Piekarz, H and Pischalnikov, Y and Podstavkov, VM and Pope, BG and Prosper, HB and Protopopescu, S and Pus̆eljić, D and Qian, J and Quintas, PZ and Raja, R and Rajagopalan, S and Ramirez, O and Rapidis,
PA and Rasmussen, L and Reucroft, S and Rijssenbeek, M and Rockwell, T and Roe, NA and Robinov, P and Ruchti, R and Rutherfoord, J and Sánchez-Hernández, A and Santoro, A and Sawyer, L and Schamberger,
RD and Schellman, H and Sculli, J and Shabalina, E and Shaffer, C and Shankar, HC and Shivpuri, RK and Shupe, M and Singh, H and Singh, JB and Sirotenko, V and Smart, W and Smith, A and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sood, PM and Sosebee,
M and Sotnikova, N and Souza, M and Spadafora, AL and Stephens, RW and Stevenson, ML and Stewart, D and Stoianova, DA and Stoker, D and Streets, K and Strovink, M and Sznajder, A and Tamburello, P and Tarazi,
J and Tartaglia, M and Thomas, TLT and Thompson, J and Trippe, TG and Tuts,
PM and Varelas, N and Varnes, EW and Vititoe, D and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, G and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Wightman, JA and Willis, S and Wimpenny, SJ and Wirjawan, JVD and Womersley, J and Won,
E and Wood, DR and Xu, H and Yamada, R and Yamin, P and Yanagisawa, C and Yang, J and Yasuda, T and Yepes, P and Yoshikawa, C and Youssef, S and Yu,
J and Yu, Y and Zhu, Q and Zhu, ZH and Zieminska, D and Zieminski, A and Zverev, EG and Zylberstejn, A},
Title = {Limits on anomalous WWγ couplings from pp → Wγ + X
events at √s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {78},
Number = {19},
Pages = {3634-3639},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.78.3634},
Abstract = {We have measured the WW? gauge boson coupling parameters
using pp → ℓνγ + X (ℓ = e,μ) events at √s=1.8
TeV. The data, corresponding to an integrated luminosity of
92.8pb-1, were collected using the DØ detector at the
Fermilab Tevatron Collider. The measured cross section times
branching ratio for pp → Wγ+ X with pγT> 10 GeV/c and
Rℓν> 0.7 is 11.3+1.7-1.5±1.5 pb, in agreement with the
standard model prediction. The 1 degree of freedom 95%
confidence level limits on individual CP-conserving
parameters are -0.93 < Δκ < 0.94 and -0.31 < λ < 0.29.
Similar limits are set on the CP-violating coupling
parameters. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.78.3634},
Key = {Abachi97d}
}
@article{fds332359,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Limits on anomalous [Formula Presented] and [Formula
Presented] couplings},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.58.031102},
Abstract = {Limits on the anomalous [Formula Presented] and [Formula
Presented] couplings are presented from a simultaneous fit
to the data samples of three gauge boson pair final states
in [Formula Presented] collisions at [Formula Presented]
[Formula Presented] production with the [Formula Presented]
boson decaying to [Formula Presented] or μν, [Formula
Presented] boson pair production with both of the [Formula
Presented] bosons decaying to [Formula Presented] or μν,
and [Formula Presented] or [Formula Presented] production
with one [Formula Presented] boson decaying to [Formula
Presented] and the other [Formula Presented] boson or the
[Formula Presented] boson decaying to two jets. Assuming
identical [Formula Presented] and [Formula Presented]
couplings, 95% C.L. limits on the anomalous couplings of
[Formula Presented] [Formula Presented] and [Formula
Presented] [Formula Presented] are obtained using a form
factor scale [Formula Presented] Limits found under other
assumptions on the relationship between the [Formula
Presented] and [Formula Presented] couplings are also
presented. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevD.58.031102},
Key = {fds332359}
}
@article{fds308202,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buescher,
V and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum,
Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev,
SV and Chen, LP and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper,
WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
D},
Title = {Limits on anomalous [formula presented] and [formula
presented] couplings from [formula presented]
production},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {62},
Number = {5},
Pages = {18},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.62.052005},
Abstract = {Limits on anomalous (Formula presented) and (Formula
presented) couplings are presented from a study of (Formula
presented) events produced in (Formula presented) collisions
at (Formula presented) Results from the analysis of data
collected using the DØ detector during the 1993–1995
Tevatron collider run at Fermilab are combined with those of
an earlier study from the 1992–1993 run. A fit to the
transverse momentum spectrum of the W boson yields direct
limits on anomalous (Formula presented) and (Formula
presented) couplings. With the assumption that the (Formula
presented) and (Formula presented) couplings are equal, we
obtain (Formula presented) (with (Formula presented) and
(Formula presented) (with (Formula presented) at the 95%
confidence level for a form-factor scale (Formula
presented). © 2000 The American Physical
Society.},
Doi = {10.1103/PhysRevD.62.052005},
Key = {fds308202}
}
@article{fds308206,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl,
OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov,
D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann,
R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
D},
Title = {Limits on quark compositeness from high energy jets in
[formula presented] collisions at 1.8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {62},
Number = {3},
Pages = {6},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.62.031101},
Abstract = {Events in (Formula presented) collisions at (Formula
presented) with total transverse energy exceeding (Formula
presented) are used to set limits on quark substructure. The
data are consistent with next-to-leading order QCD
calculations. We set a lower limit of (Formula presented) at
95% confidence on the energy scale (Formula presented) for
compositeness in quarks, assuming a model with a left-left
isoscalar contact interaction term. The limits on (Formula
presented) are found to be insensitive to the sign of the
interference term in the Lagrangian. © 2000 The American
Physical Society.},
Doi = {10.1103/PhysRevD.62.031101},
Key = {fds308206}
}
@article{fds307892,
Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams,
DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna,
P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M and Anduaga,
XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
R},
Title = {Limits on the production of the standard model Higgs boson
in pp collisions at √s=7 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {71},
Number = {9},
Pages = {1-30},
Publisher = {Springer Nature},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1728-9},
Abstract = {A search for the Standard Model Higgs boson at the Large
Hadron Collider (LHC) running at a centre-of-mass energy of
7 TeV is reported, based on a total integrated luminosity of
up to 40 pb-1 collected by the ATLAS detector in 2010.
Several Higgs boson decay channels: H→γγ,
H→ZZ(*)→ℓℓℓℓ, H→ZZ→ℓℓνν,
H→ZZ→ℓℓqq, H→WW(*)→ℓνℓν and
H→WW→ℓνqq (ℓ is e, μ) are combined in a mass range
from 110 GeV to 600 GeV. The highest sensitivity is achieved
in the mass range between 160 GeV and 170 GeV, where the
expected 95% CL exclusion sensitivity is at Higgs boson
production cross sections 2. 3 times the Standard Model
prediction. Upper limits on the cross section for its
production are determined. Models with a fourth generation
of heavy leptons and quarks with Standard Model-like
couplings to the Higgs boson are also investigated and are
excluded at 95% CL for a Higgs boson mass in the range from
140 GeV to 185 GeV. © 2011 CERN for the benefit of the
ATLAS collaboration.},
Doi = {10.1140/epjc/s10052-011-1728-9},
Key = {fds307892}
}
@booklet{Abbott98b,
Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
Alves and N. Amos and E. W. Anderson and R. Astur and M. M.
Baarmand and L. Babukhadia and A. Baden and V. Balamurali and J. Balderston},
Title = {Limits on WW gamma and WWZ couplings from W boson pair
production},
Journal = {Physical Review D},
Volume = {5805},
Number = {5},
Pages = {art. no. -- 051101},
Year = {1998},
Month = {September},
Key = {Abbott98b}
}
@booklet{Abbott97b,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt,
A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del’signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
M and Fatyga, MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y},
Title = {Limits on WWZ and WWγ couplings from p¯p → ev
jjX Events at √s=1.8TeV},
Journal = {Physical Review Letters},
Volume = {79},
Number = {8},
Pages = {1441-1446},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.1441},
Abstract = {We present limits on anomalous WWZ and WWα couplings from a
search for WW and WZ production in p¯p collisions at √
s=1.8TeV. We use p¯p → ev jjX events recorded with the D0
detector at the Fermilab Tevatron Collider during the
1992–1995 run. The data sample corresponds to an
integrated luminosity of 96.0±5.1pb−1. Assuming identical
WWZ and WWα coupling parameters, the 95% C.L. limits on the
CP−conserving couplings are −0.33 < λ < 0.36 (Δk=0)
and −0.43 < Δk < 0.59 (λ=0), for a form factor scale =
⋀ 2.0TeV. Limits based on other assumptions are also
presented. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.79.1441},
Key = {Abbott97b}
}
@article{fds308234,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and Signore, KD and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Loreto, GD and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Geld, TL and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Glenn, S and Gobbi, B and Goldschmidt, A and Gómez, B and Gómez, G and Goncharov,
PI and Solís, JLG and Gordon, H and Goss, LT and Gounder, K and Goussiou,
A and Graf, N and Grannis, PD and Green, DR and Greenlee, H and Grinstein,
S and Grudberg, P and Grünendahl, S and Guglielmo, G and Guida, JA and Guida, JM and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez,
P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn,
KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hedin, D and Heinson, AP and Heintz, U and Hernández-Montoya, R and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hsieh, F and Ting, H and Tong, H and Huehn, T and Ito, AS and James, E and Jaques, J and Jerger, SA and Jesik, R and Jiang, JZY and Joffe-Minor, T and Johari, H and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Jun, SY and Jung, CK and Kahn, S and Kalbfleisch, G and Kang, JS and Karmanov, D and Karmgard, D and Kehoe, R and Kelly, ML and Kim, CL and Kim,
SK and Klima, B and Klopfenstein, C and Kohli, JM and Koltick, D and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kourlas, J and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kuleshov, S and Kunori, S and Landry, F and Landsberg, G and Lauer, B and Leflat, A and Li, H and Li, J and Li-Demarteau, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Liu, YC and Lobkowicz, F and Loken, SC and Lökös, S and Lueking, L and Lyon, AL and Maciel, AKA and Madaras, RJ and Madden, R and Magaña-Mendoza, L and Manankov, V and Mani, S and Mao,
HS and Markeloff, R and Marshall, T and Martin, MI and Mauritz, KM and May,
B and Mayorov, AA and McCarthy, R and McDonald, J and McKibben, T and McKinley, J and McMahon, T and Melanson, HL and Merkin, M and Merritt,
KW and Miettinen, H and Mincer, A and Mishra, CS and Mokhov, N and Mondal,
NK and Montgomery, HE and Mooney, P and Motta, HD and Murphy, C and Nang,
F and Narain, M and Narasimham, VS and Narayanan, A and Neal, HA and Negret, JP and Nemethy, P and Norman, D and Oesch, L and Oguri, V and Oliveira, E and Oltman, E and Oshima, N and Owen, D and Padley, P and Para,
A and Park, YM and Partridge, R and Parua, N and Paterno, M and Pawlik, B and Perkins, J and Peters, M and Piegaia, R and Piekarz, H and Pischalnikov,
Y and Pope, BG and Prosper, HB and Protopopescu, S and Qian, J and Quintas,
PZ and Raja, R and Rajagopalan, S and Ramirez, O and Rasmussen, L and Reucroft, S and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov,
P and Ruchti, R and Rutherfoord, J and Sánchez-Hernández, A and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Sculli, J and Shabalina, E and Shaffer, C and Shankar, HC and Shivpuri,
RK and Shupe, M and Singh, H and Singh, JB and Sirotenko, V and Smart, W and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder,
S and Solomon, J and Sosebee, M and Sotnikova, N and Souza, M and Spadafora, AL and Steinbrück, G and Stephens, RW and Stevenson, ML and Stewart, D and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova,
DA and Strauss, M and Streets, K and Strovink, M and Sznajder, A and Tamburello, P and Tarazi, J and Tartaglia, M and Thomas, TLT and Thompson, J and Trippe, TG and Tuts, PM and Varelas, N and Varnes, EW and Vititoe, D and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, G and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White,
JT and Wightman, JA and Willis, S and Wimpenny, SJ and Wirjawan, JVD and Womersley, J and Won, E and Wood, DR and Xu, H and Yamada, R and Yamin, P and Yang, J and Yasuda, T and Yepes, P and Yoshikawa, C and Youssef, S and Yu,
J and Yu, Y and Zhou, Z and Zhu, ZH and Zieminska, D and Zieminski, A and Zverev, EG and Zylberstejn, A},
Title = {Limits on WWγ and WWZ couplings from IV boson pair
production},
Journal = {Physical Review D},
Volume = {58},
Number = {5},
Pages = {DUMMY1},
Year = {1998},
Abstract = {The results of a search for W boson pair production in pp
collisions at √s= 1.8 TeV with subsequent decay to eμ,
ee, and μμ channels are presented. Five candidate events
are observed with an expected background of 3.1 ±0.4 events
for an integrated luminosity of approximately 97 pb-1.
Limits on the anomalous couplings are obtained from a
maximum likelihood fit of the ET spectra of the leptons in
the candidate events. Assuming identical WWγ and WWZ
couplings, the 95% C.L. limits are -0.62<Δκ<0.77 (X.
= 0) and -0.53<λ <0.56 (Δκ=0) for a form factor
scale Λ= 1.5 TeV. © 1998 The American Physical
Society.},
Key = {fds308234}
}
@article{fds308233,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Limits on [Formula Presented] and [Formula Presented]
couplings from [Formula Presented] boson pair
production},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {5},
Pages = {511011-511016},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
ISSN = {0556-2821},
url = {http://dx.doi.org/10.1103/PhysRevD.58.051101},
Abstract = {The results of a search for [Formula Presented] boson pair
production in [Formula Presented] collisions at [Formula
Presented] with subsequent decay to [Formula Presented]
[Formula Presented] and μμ channels are presented. Five
candidate events are observed with an expected background of
[Formula Presented] events for an integrated luminosity of
approximately [Formula Presented] Limits on the anomalous
couplings are obtained from a maximum likelihood fit of the
[Formula Presented] spectra of the leptons in the candidate
events. Assuming identical [Formula Presented] and [Formula
Presented] couplings, the 95% C.L. limits are [Formula
Presented] [Formula Presented] and [Formula Presented]
[Formula Presented] [Formula Presented] for a form factor
scale [Formula Presented]. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevD.58.051101},
Key = {fds308233}
}
@article{fds356026,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Artz, S and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak,
L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertram, IA and Bessidskaia Bylund and O and Besson,
N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai, P and Bi, R and Bianchi, RM and Biebel,
O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner,
R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko,
D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carter, JWS and Casado, MP and Casha,
AF and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Chytka, L and Cieri, D and Ciesla, KM and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio,
M},
Title = {Longitudinal Flow Decorrelations in Xe+Xe Collisions at
sqrt[s_{NN}]=5.44 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {126},
Number = {12},
Pages = {122301},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.126.122301},
Abstract = {The first measurement of longitudinal decorrelations of
harmonic flow amplitudes v_{n} for n=2-4 in Xe+Xe collisions
at sqrt[s_{NN}]=5.44 TeV is obtained using
3 μb^{-1} of data with the ATLAS detector at the LHC.
The decorrelation signal for v_{3} and v_{4} is found to be
nearly independent of collision centrality and transverse
momentum (p_{T}) requirements on final-state particles, but
for v_{2} a strong centrality and p_{T} dependence is seen.
When compared with the results from Pb+Pb collisions at
sqrt[s_{NN}]=5.02 TeV, the longitudinal decorrelation
signal in midcentral Xe+Xe collisions is found to be larger
for v_{2}, but smaller for v_{3}. Current hydrodynamic
models reproduce the ratios of the v_{n} measured in Xe+Xe
collisions to those in Pb+Pb collisions but fail to describe
the magnitudes and trends of the ratios of longitudinal flow
decorrelations between Xe+Xe and Pb+Pb. The results on the
system-size dependence provide new insights and an important
lever arm to separate effects of the longitudinal structure
of the initial state from other early and late time effects
in heavy-ion collisions.},
Doi = {10.1103/physrevlett.126.122301},
Key = {fds356026}
}
@article{fds321073,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Luminosity determination in pp collisions at [Formula: see
text] = 8 TeV using the ATLAS detector at the
LHC.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {12},
Pages = {653},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4466-1},
Abstract = {The luminosity determination for the ATLAS detector at the
LHC during pp collisions at [Formula: see text] 8 TeV in
2012 is presented. The evaluation of the luminosity scale is
performed using several luminometers, and comparisons
between these luminosity detectors are made to assess the
accuracy, consistency and long-term stability of the
results. A luminosity uncertainty of [Formula: see text] is
obtained for the [Formula: see text] of pp collision data
delivered to ATLAS at [Formula: see text] 8 TeV in
2012.},
Doi = {10.1140/epjc/s10052-016-4466-1},
Key = {fds321073}
}
@article{fds373905,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Dos Santos and SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH},
Title = {Luminosity determination in pp collisions at √s=13 TeV
using the ATLAS detector at the LHC},
Journal = {European Physical Journal C},
Volume = {83},
Number = {10},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11747-w},
Abstract = {The luminosity determination for the ATLAS detector at the
LHC during Run 2 is presented, with pp collisions at a
centre-of-mass energy s=13 TeV. The absolute luminosity
scale is determined using van der Meer beam separation scans
during dedicated running periods in each year, and
extrapolated to the physics data-taking regime using
complementary measurements from several luminosity-sensitive
detectors. The total uncertainties in the integrated
luminosity for each individual year of data-taking range
from 0.9% to 1.1%, and are partially correlated between
years. After standard data-quality selections, the full
Run 2 pp data sample corresponds to an integrated
luminosity of 140.1 ± 1.2 fb - 1 , i.e. an uncertainty of
0.83%. A dedicated sample of low-pileup data recorded in
2017–2018 for precision Standard Model physics
measurements is analysed separately, and has an integrated
luminosity of 338.1 ± 3.1 pb - 1 .},
Doi = {10.1140/epjc/s10052-023-11747-w},
Key = {fds373905}
}
@article{fds310263,
Author = {Hinchliffe, I and Kotwal, A and Mangano, ML and Quigg, C and Wang,
LT},
Title = {Luminosity goals for a 100-TeV pp collider},
Journal = {International Journal of Modern Physics A},
Volume = {30},
Number = {23},
Pages = {1544002-1544002},
Publisher = {World Scientific Pub Co Pte Lt},
Year = {2015},
Month = {August},
ISSN = {0217-751X},
url = {http://dx.doi.org/10.1142/S0217751X15440029},
Abstract = {We consider diverse examples of science goals that provide a
framework to assess luminosity goals for a future 100-TeV
proton-proton collider.},
Doi = {10.1142/S0217751X15440029},
Key = {fds310263}
}
@article{fds227090,
Author = {Ian Hinchliffe and Ashutosh Kotwal and Michelangelo L. Mangano and Chris Quigg and Lian-Tao Wang},
Title = {Luminosity goals for a 100-TeV pp collider},
Journal = {Int.J.Mod.Phys. A},
Volume = {30},
Number = {1544002},
Year = {2015},
Month = {April},
Key = {fds227090}
}
@article{fds307539,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Mass and lifetime measurements of bottom and charm baryons
in p p ̄ collisions at s =1.96TeV MASS and LIFETIME
MEASUREMENTS of BOTTOM and ⋯ T. AALTONEN},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {April},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072014},
Abstract = {We report on mass and lifetime measurements of several
ground state charmed and bottom baryons, using a data sample
corresponding to 9.6fb-1 from pp̄ collisions at s=1.96TeV
and recorded with the Collider Detector at Fermilab. Baryon
candidates are reconstructed from data collected with an
online event selection designed for the collection of
long-lifetime heavy-flavor decay products and a second event
selection designed to collect J/ ψ→μ+μ- candidates.
First evidence for the process Ωb-→Ωc0π- is presented
with a significance of 3.3σ. We measure the following
baryon masses: M(Ξc0)=2470.85±0.24(stat)
±0.55(syst)MeV/c2,M(Ξc+)=2468.00±0.18(stat)±0.51(syst)
MeV/c2,M(Λb)=5620.15±0.31(stat)±0.47(syst)MeV/c2,M(Ξb-)=
5793.4±1.8(stat)±0.7(syst)MeV/c2,M(Ξb0)=5788.7±4.3(stat)
±1.4(syst)MeV/c2,andM(Ωb-)=6047.5±3.8(stat)±0.6(syst)
MeV/c2.The isospin splitting of the Ξb-,0 states is found
to be M(Ξb-)-M(Ξb0)=4.7±4.7(stat)±0.7(syst)MeV/c2. The
isospin splitting of the Ξc0,+ states is found to be
M(Ξc0)-M(Ξc+)=2. 85±0.30(stat)±0.04(syst)MeV/c2. The
following lifetime measurements are made:
τ(Λb)=1.565±0.035(stat)±0. 020(syst)ps,τ(Ξb-)=1.32±0.14(stat)±0.02(syst)ps,
τ(Ωb-)=1.66-0.40+0.53(stat)±0.02(syst)ps. © 2014
American Physical Society.},
Doi = {10.1103/PhysRevD.89.072014},
Key = {fds307539}
}
@article{fds346185,
Author = {Agrawal, S and Puthia, A and Kotwal, A and Tilak, R and Kunte, R and Kushwaha, AS},
Title = {Mass scabies management in an orphanage of rural community:
An experience.},
Journal = {Medical journal, Armed Forces India},
Volume = {68},
Number = {4},
Pages = {403-406},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.02.014},
Doi = {10.1016/j.mjafi.2012.02.014},
Key = {fds346185}
}
@article{fds308096,
Author = {Acosta, and D, and others},
Title = {Measurement of $b$ hadron masses in exclusive $J/\psi$
decays with the CDF detector},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {20},
Pages = {202001},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.202001},
Abstract = {We measure the masses of $b$ hadrons in exclusively
reconstructed final states containing a $J/\psi\to\mu^-\mu^+$
decay using $\rm 220 pb^{-1}$ of data collected by the CDF
II experiment. We find: m(B^+) = 5279.10 \pm 0.41_{(stat.)}
\pm 0.36_{(sys.)} MeVcc, m(B^0) = 5279.63 \pm 0.53_{(stat.)}
\pm 0.33_{(sys.)} MeVcc, m(B^0_s) = 5366.01 \pm
0.73_{(stat.)} \pm 0.33_{(sys.)} MeVcc, m(\Lambda^0_b) =
5619.7 \pm 1.2_{(stat.)} \pm 1.2_{(sys.)} MeVcc. m(B^+) -
m(B^0) = -0.53 \pm 0.67_{(stat.)} \pm 0.14_{(sys.)} MeVcc,
m(B^0_s) - m(B^0) = 86.38 \pm 0.90_{(stat.)} \pm
0.06_{(sys.)} MeVcc m(\Lambda^0_b) - m(B^0) = 339.2 \pm
1.4_{(stat.)} \pm 0.1_{(sys.)} MeVcc. The measurements of
the $B^0_s$, $\Lambda^0_b$ mass, $m(B^0_s)-m(B^0)$ and
$m(\Lambda^0_b)-m(B^0)$ mass difference are of better
precision than the current world averages.},
Doi = {10.1103/physrevlett.96.202001},
Key = {fds308096}
}
@article{fds307877,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of $t\overline{t}$ spin correlation in
$p\overline{p}$ collisions using the CDF II detector at the
Tevatron},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {3},
Pages = {031104},
Publisher = {American Physical Society},
Year = {2011},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.83.031104},
Abstract = {The tt̄ spin correlation at production is a fundamental
prediction of QCD and a potentially incisive test of new
physics coupled to top quarks. We measure the tt̄ spin
state in pp̄ collisions at √s=1.96TeV using 1001
candidate events in the lepton plus jets decay channel
reconstructed in the CDF II detector. In the helicity basis,
for a top-quark mass of 172.5GeV/c2, we find a spin
correlation coefficient κ=0.60±0.50(stat)±0. 16(syst),
consistent with the QCD prediction, κ 0.40. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.031104},
Key = {fds307877}
}
@article{fds307920,
Author = {Aaltonen, and T, and others},
Title = {Measurement of $Z\gamma{}$ production in $pp[over
\ifmmode\bar\else\textasciimacron\fi{}]$ collisions at
$\sqrt{s}=1.96\,\,TeV$},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {3},
Pages = {031103},
Publisher = {American Physical Society},
Year = {2010},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.82.031103},
Abstract = {The production rate and kinematics of photons produced in
association with Z bosons are studied using 2fb-1 of pp̄
collision data collected at the Collider Detector at
Fermilab. The cross section for pp̄→"+-γ+X (where the
leptons " are either muons or electrons with dilepton mass
M>40GeV/c2, and where the photon has transverse energy
ETγ>7GeV and is well separated from the leptons) is
4.6±0.2(stat)±0.3(syst)±0.3(lum)pb, which is consistent
with standard model expectations. We use the photon ET
distribution from Zγ events where the Z has decayed to
μ+μ -, e+e-, or νν̄ to set limits on anomalous (non
standard model) trilinear couplings between photons and Z
bosons. © 2010 The American Physical Society.},
Doi = {10.1103/PhysRevD.82.031103},
Key = {fds307920}
}
@article{fds307852,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of ${b}$ Hadron Lifetimes in Exclusive Decays
Containing a ${J}/\psi$ in $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {12},
Pages = {121804},
Publisher = {American Physical Society},
Year = {2011},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.121804},
Abstract = {We report on a measurement of b-hadron lifetimes in the
fully reconstructed decay modes B(+)→J/ψK(+),
B⁰→J/ψK*(892)⁰, B⁰→J/ψK(s)⁰, and
Λ(b)⁰→J/ψΛ⁰ using data corresponding to an
integrated luminosity of 4.3 fb⁻¹, collected by the CDF
II detector at the Fermilab Tevatron. The measured lifetimes
are τ(B(+))=[1.639±0.009(stat)±0.009(syst)] ps,
τ(B⁰)=[1.507±0.010(stat)±0.008(syst)] ps, and
τ(Λ(b)⁰)=[1.537±0.045(stat)±0.014(syst)] ps. The
lifetime ratios are τ(B(+))/τ(B⁰)=[1.088±0.009(stat)±0.004(syst)]
and τ(Λ(b)⁰)/τ(B⁰)=[1.020±0.030(stat)±0.008(syst)].
These are the most precise determinations of these
quantities from a single experiment.},
Doi = {10.1103/PhysRevLett.106.121804},
Key = {fds307852}
}
@article{fds307604,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach,
B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli,
F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behar Harpaz and S and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C},
Title = {Measurement of kT splitting scales in
W→ℓν events at [Formula: see text] with
the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {5},
Pages = {2432},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2432-8},
Abstract = {A measurement of splitting scales, as defined by the
<i>k</i><sub>T</sub> clustering algorithm, is presented for
final states containing a <i>W</i> boson produced in
proton-proton collisions at a centre-of-mass energy of
7 TeV. The measurement is based on the full 2010 data
sample corresponding to an integrated luminosity of
36 pb<sup>-1</sup> which was collected using the ATLAS
detector at the CERN Large Hadron Collider. Cluster
splitting scales are measured in events containing <i>W</i>
bosons decaying to electrons or muons. The measurement
comprises the four hardest splitting scales in a
<i>k</i><sub>T</sub> cluster sequence of the hadronic
activity accompanying the <i>W</i> boson, and ratios of
these splitting scales. Backgrounds such as multi-jet and
top-quark-pair production are subtracted and the results are
corrected for detector effects. Predictions from various
Monte Carlo event generators at particle level are compared
to the data. Overall, reasonable agreement is found with all
generators, but larger deviations between the predictions
and the data are evident in the soft regions of the
splitting scales.},
Doi = {10.1140/epjc/s10052-013-2432-8},
Key = {fds307604}
}
@article{fds307770,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi,
E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W},
Title = {Measurement of τ polarization in
W→τν decays with the ATLAS detector in
pp collisions at [Formula: see text].},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {72},
Number = {7},
Pages = {2062},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2062-6},
Abstract = {In this paper, a measurement of <i>τ</i> polarization in
<i>W</i>→<i>τν</i> decays is presented. It is measured
from the energies of the decay products in hadronic
<i>τ</i> decays with a single final state charged particle.
The data, corresponding to an integrated luminosity of
24 pb<sup>-1</sup>, were collected by the ATLAS experiment
at the Large Hadron Collider in 2010. The measured value of
the <i>τ</i> polarization is [Formula: see text], in
agreement with the Standard Model prediction, and is
consistent with a physically allowed 95 % CL
interval [-1,-0.91]. Measurements of <i>τ</i> polarization
have not previously been made at hadron colliders.},
Doi = {10.1140/epjc/s10052-012-2062-6},
Key = {fds307770}
}
@article{fds356554,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Measurement of angular and momentum distributions of charged
particles within and around jets in Pb+Pb and pp collisions
at sNN =5.02 TeV with the ATLAS detector},
Journal = {Physical Review C},
Volume = {100},
Number = {6},
Year = {2019},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevC.100.064901},
Abstract = {Studies of the fragmentation of jets into charged particles
in heavy-ion collisions can provide information about the
mechanism of jet quenching by the hot and dense QCD matter
created in such collisions, the quark-gluon plasma. This
paper presents a measurement of the angular distribution of
charged particles around the jet axis in sNN=5.02 TeV Pb+Pb
and pp collisions, using the ATLAS detector at the LHC. The
Pb+Pb and pp data sets have integrated luminosities of
0.49nb-1 and 25pb-1, respectively. The measurement is
performed for jets reconstructed with the anti-kt algorithm
with radius parameter R=0.4 and is extended to an angular
distance of r=0.8 from the jet axis. Results are presented
as a function of Pb+Pb collision centrality and distance
from the jet axis for charged particles with transverse
momenta in the 1- to 63-GeV range, matched to jets with
transverse momenta in the 126- to 316-GeV range and an
absolute value of jet rapidity of less than 1.7.
Modifications to the measured distributions are quantified
by taking a ratio to the measurements in pp collisions.
Yields of charged particles with transverse momenta below 4
GeV are observed to be increasingly enhanced as a function
of angular distance from the jet axis, reaching a maximum at
r=0.6. Charged particles with transverse momenta above 4 GeV
have an enhanced yield in Pb+Pb collisions in the jet core
for angular distances up to r=0.05 from the jet axis, with a
suppression at larger distances.},
Doi = {10.1103/PhysRevC.100.064901},
Key = {fds356554}
}
@article{fds307611,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurement of angular correlations in Drell–Yan lepton
pairs to probe Z/γ⁎ boson transverse momentum
at √s=7 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {720},
Number = {1-3},
Pages = {32-51},
Publisher = {Elsevier BV},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.054},
Abstract = {A measurement of angular correlations in Drell–Yan lepton
pairs via the ϕη⁎ observable is presented. This variable
probes the same physics as the Z/γ⁎ boson transverse
momentum with a better experimental resolution. The
Z/γ⁎→e+e− and Z/γ⁎→μ+μ− decays produced in
proton–proton collisions at a centre-of-mass energy of
sqrts=7 TeV are used. The data were collected with the ATLAS
detector at the LHC and correspond to an integrated
luminosity of 4.6 fb−1. Normalised differential cross
sections as a function of ϕη⁎ are measured separately
for electron and muon decay channels. These channels are
then combined for improved accuracy. The cross section is
also measured double differentially as a function of ϕη⁎
for three independent bins of the Z boson rapidity. The
results are compared to QCD calculations and to predictions
from different Monte Carlo event generators. The data are
reasonably well described, in all measured Z boson rapidity
regions, by resummed QCD predictions combined with
fixed-order perturbative QCD calculations or by some Monte
Carlo event generators. The measurement precision is
typically better by one order of magnitude than present
theoretical uncertainties.},
Doi = {10.1016/j.physletb.2013.01.054},
Key = {fds307611}
}
@article{fds351087,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R},
Title = {Measurement of azimuthal anisotropy of muons from charm and
bottom hadrons in Pb+Pb collisions at sNN=5.02
TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {807},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2020.135595},
Abstract = {Azimuthal anisotropies of muons from charm and bottom hadron
decays are measured in Pb+Pb collisions at sNN=5.02TeV. The
data were collected with the ATLAS detector at the Large
Hadron Collider in 2015 and 2018 with integrated
luminosities of 0.5nb−1 and 1.4nb−1, respectively. The
kinematic selection for heavy-flavor muons requires
transverse momentum 4<pT<30GeV and pseudorapidity |η|<2.0.
The dominant sources of muons in this pT range are
semi-leptonic decays of charm and bottom hadrons. These
heavy-flavor muons are separated from light-hadron decay
muons and punch-through hadrons using the momentum imbalance
between the measurements in the tracking detector and in the
muon spectrometers. Azimuthal anisotropies, quantified by
flow coefficients, are measured via the event-plane method
for inclusive heavy-flavor muons as a function of the muon
pT and in intervals of Pb+Pb collision centrality.
Heavy-flavor muons are separated into contributions from
charm and bottom hadron decays using the muon transverse
impact parameter with respect to the event primary vertex.
Non-zero elliptic (v2) and triangular (v3) flow coefficients
are extracted for charm and bottom muons, with the charm
muon coefficients larger than those for bottom muons for all
Pb+Pb collision centralities. The results indicate
substantial modification to the charm and bottom quark
angular distributions through interactions in the
quark-gluon plasma produced in these Pb+Pb collisions, with
smaller modifications for the bottom quarks as expected
theoretically due to their larger mass.},
Doi = {10.1016/j.physletb.2020.135595},
Key = {fds351087}
}
@article{fds348980,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling,
J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assahsah,
J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay,
NB and Atmani, H and Augsten, K and Avolio, G and Avramidou, R and Ayoub,
MK and Azoulay, AM and Azuelos, G and Bachacou, H and Bachas, K and Backes,
M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin,
EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barsov, S and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertram, IA and Bessidskaia Bylund and O and Besson, N and Bethani,
A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya,
DS and Bhattarai, P and Bi, R and Bianchi, RM and Biebel, O and Biedermann,
D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton,
CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carter, JWS and Casado, MP and Casha, AF and Casper, DW and Castelijn,
R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, SK and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen,
Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias,
TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu,
MC},
Title = {Measurement of Azimuthal Anisotropy of Muons from Charm and
Bottom Hadrons in pp Collisions at sqrt[s]=13 TeV with
the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {124},
Number = {8},
Pages = {082301},
Year = {2020},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.124.082301},
Abstract = {The elliptic flow of muons from the decay of charm and
bottom hadrons is measured in pp collisions at
sqrt[s]=13 TeV using a data sample with an integrated
luminosity of 150 pb^{-1} recorded by the ATLAS
detector at the LHC. The muons from heavy-flavor decay are
separated from light-hadron decay muons using momentum
imbalance between the tracking and muon spectrometers. The
heavy-flavor decay muons are further separated into those
from charm decay and those from bottom decay using the
distance-of-closest-approach to the collision vertex. The
measurement is performed for muons in the transverse
momentum range 4-7 GeV and pseudorapidity range |η|<2.4. A
significant nonzero elliptic anisotropy coefficient v_{2} is
observed for muons from charm decays, while the v_{2} value
for muons from bottom decays is consistent with zero within
uncertainties.},
Doi = {10.1103/physrevlett.124.082301},
Key = {fds348980}
}
@article{fds351560,
Author = {Acosta, and D, and others},
Title = {Measurement of B(t --> W b)/B(t --> W q) at the Collider
Detector at Fermilab},
Journal = {Phys. Rev. Lett.},
Volume = {95},
Number = {10},
Pages = {102002},
Year = {2005},
url = {http://dx.doi.org/10.1103/physrevlett.95.102002},
Abstract = {http://arxiv.org/abs/hep-ex/0505091},
Doi = {10.1103/physrevlett.95.102002},
Key = {fds351560}
}
@article{fds310396,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and (CDF
Collaboration)},
Title = {Measurement of B(t→Wb)/B(t→Wq) in top-quark-pair decays
using dilepton events and the full CDF Run II data
set.},
Journal = {Physical review letters},
Volume = {112},
Number = {22},
Pages = {221801},
Year = {2014},
Month = {June},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.112.221801},
Abstract = {We present a measurement of the ratio of the top-quark
branching fractions R=B(t→Wb)/B(t→Wq), where q
represents any quark flavor, in events with two charged
leptons, imbalance in total transverse energy, and at least
two jets. The measurement uses proton-antiproton collision
data at center-of-mass energy 1.96 TeV, corresponding to an
integrated luminosity of 8.7 fb^{-1} collected with the
Collider Detector at Fermilab during Run II of the Tevatron.
We measure R to be 0.87±0.07, and extract the magnitude of
the top-bottom quark coupling to be |V_{tb}|=0.93±0.04,
assuming three generations of quarks. Under these
assumptions, a lower limit of |V_{tb}|>0.85(0.87) at 95%
(90%) credibility level is set.},
Doi = {10.1103/physrevlett.112.221801},
Key = {fds310396}
}
@article{fds356725,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurement of b-hadron pair production with the ATLAS
detector in proton-proton collisions at √s=8
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {11},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2017)062},
Abstract = {A measurement of b-hadron pair production is presented,
based on a data set corresponding to an integrated
luminosity of 11.4 fb−1 of proton-proton collisions
recorded at s=8 TeV with the ATLAS detector at the LHC.
Events are selected in which a b-hadron is reconstructed in
a decay channel containing J/ψ → μμ, and a second
b-hadron is reconstructed in a decay channel containing a
muon. Results are presented in a fiducial volume defined by
kinematic requirements on three muons based on those used in
the analysis. The fiducial cross section is measured to be
17.7 ± 0.1(stat.) ± 2.0(syst.) nb. A number of normalised
differential cross sections are also measured, and compared
to predictions from the Pythia8, Herwig++,
MadGraph5_aMC@NLO+Pythia8 and Sherpa event generators,
providing new constraints on heavy flavour
production.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP11(2017)062},
Key = {fds356725}
}
@article{fds361168,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
Title = {Measurement of b-quark fragmentation properties in jets
using the decay B ± → J/ψK ± in
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {12},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2021)131},
Abstract = {The fragmentation properties of jets containing b-hadrons
are studied using charged B mesons in 139 fb−1 of pp
collisions at s = 13 TeV, recorded with the ATLAS detector
at the LHC during the period from 2015 to 2018. The B mesons
are reconstructed using the decay of B± into J/ψK±, with
the J/ψ decaying into a pair of muons. Jets are
reconstructed using the anti-kt algorithm with radius
parameter R = 0.4. The measurement determines the
longitudinal and transverse momentum profiles of the
reconstructed B hadrons with respect to the axes of the jets
to which they are geometrically associated. These
distributions are measured in intervals of the jet
transverse momentum, ranging from 50 GeV to above 100 GeV.
The results are corrected for detector effects and compared
with several Monte Carlo predictions using different parton
shower and hadronisation models. The results for the
longitudinal and transverse profiles provide useful inputs
to improve the description of heavy-flavour fragmentation in
jets. [Figure not available: see fulltext.].},
Doi = {10.1007/JHEP12(2021)131},
Key = {fds361168}
}
@article{fds307886,
Author = {Aaltonen, TEA},
Title = {Measurement of branching ratio and ${B}_{s}^{0}$ lifetime in
the decay ${B}_{s}^{0}\rightarrow{J}/\psi{f}_{0}(980)$ at
{CDF}},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {5},
Pages = {052012},
Publisher = {American Physical Society},
Year = {2011},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.84.052012},
Abstract = {We present a study of Bs0 decays to the CP-odd final state
J/ψf 0(980) with J/ψ→μ+μ- and f 0(980)→π+π-. Using
pp̄ collision data with an integrated luminosity of 3.8fb-1
collected by the CDF II detector at the Tevatron we measure
a Bs0 lifetime of τ(Bs0→J/ψf0(980))=1.70-0.11+0.12(stat)±0.03(syst)
ps. This is the first measurement of the Bs0 lifetime in a
decay to a CP eigenstate and corresponds in the standard
model to the lifetime of the heavy Bs0 eigenstate. We also
measure the product of branching fractions of
Bs0→J/ψf0(980) and f0(980)→π +π- relative to the
product of branching fractions of Bs0→J/ψ and →K+K- to
be Rf0 /=0.257±0.020(stat)±0.014(syst), which is the most
precise determination of this quantity to date. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.84.052012},
Key = {fds307886}
}
@article{fds307705,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of Bs0→Ds(*)+Ds(*)- branching
ratios.},
Journal = {Physical review letters},
Volume = {108},
Number = {20},
Pages = {201801},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.201801},
Abstract = {The decays Bs0→Ds(*)+Ds(*)- are reconstructed in a data
sample corresponding to an integrated luminosity of
6.8 fb-1 collected by the CDF II detector at the
Tevatron pp[over ¯] collider. All decay modes are observed
with a significance of more than 10σ, and we measure the
Bs0 production rate times Bs0→Ds(*)+Ds(*)- branching
ratios relative to the normalization mode B0→Ds+D-to be
0.183±0.021±0.017 for Bs0→Ds+Ds-, 0.424±0.046±0.035
for Bs0→Ds*±Ds^∓, 0.654±0.072±0.065 for
Bs0→Ds*+Ds*-, and 1.261±0.095±0.112 for the inclusive
decay Bs0→Ds(*)+Ds(*)-, where the uncertainties are
statistical and systematic. These results are the most
precise single measurements to date and provide important
constraints for indirect searches for nonstandard model
physics in Bs0 mixing.},
Doi = {10.1103/physrevlett.108.201801},
Key = {fds307705}
}
@article{fds310287,
Author = {Aaltonen, T and Albrow, MG and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri,
A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher,
R},
Title = {Measurement of central exclusive π+π- production in p p ¯
collisions at s =0.9 and 1.96 TeV at CDF MEASUREMENT of
CENTRAL EXCLUSIVE π+π- ... T. AALTONEN et
al.},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.91.091101},
Abstract = {We measure exclusive π+π- production in proton-antiproton
collisions at center-of-mass energies s=0.9 and 1.96 TeV in
the Collider Detector at Fermilab. We select events with two
oppositely charged particles, assumed to be pions, with
pseudorapidity |η|<1.3 and with no other particles detected
in |η|<5.9. We require the π+π- system to have rapidity
|y|<1.0. The production mechanism of these events is
expected to be dominated by double pomeron exchange, which
constrains the quantum numbers of the central state. The
data are potentially valuable for isoscalar meson
spectroscopy and for understanding the pomeron in a region
of transition between nonperturbative and perturbative
quantum chromodynamics. The data extend up to dipion mass
M(π+π-)=5000MeV/c2 and show resonance structures
attributed to f0 and f2(1270) mesons. From the π+π- and
K+K- spectra, we place upper limits on exclusive χc0(3415)
production.},
Doi = {10.1103/PhysRevD.91.091101},
Key = {fds310287}
}
@article{fds356758,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurement of charged-particle distributions sensitive to
the underlying event in √s=13 TeV proton-proton collisions
with the ATLAS detector at the LHC},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {3},
Year = {2017},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2017)157},
Abstract = {We present charged-particle distributions sensitive to the
underlying event, measured by the ATLAS detector in
proton-proton collisions at a centre-of-mass energy of 13
TeV, in low-luminosity Large Hadron Collider fills
corresponding to an integrated luminosity of 1.6 nb−1. The
distributions were constructed using charged particles with
absolute pseudorapidity less than 2.5 and with transverse
momentum greater than 500 MeV, in events with at least one
such charged particle with transverse momentum above 1 GeV.
These distributions characterise the angular distribution of
energy and particle flows with respect to the charged
particle with highest transverse momentum, as a function of
both that momentum and of charged-particle multiplicity. The
results have been corrected for detector effects and are
compared to the predictions of various Monte Carlo event
generators, experimentally establishing the level of
underlying-event activity at LHC Run 2 energies and
providing inputs for the development of event generator
modelling. The current models in use for UE modelling
typically describe this data to 5% accuracy, compared with
data uncertainties of less than 1%.[Figure not available:
see fulltext.]},
Doi = {10.1007/JHEP03(2017)157},
Key = {fds356758}
}
@article{fds307586,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurement of charged-particle event shape variables in
inclusive √(s)=7 TeV proton-proton interactions with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.88.032004},
Abstract = {The measurement of charged-particle event shape variables is
presented in inclusive inelastic pp collisions at a
center-of-mass energy of 7 TeV using the ATLAS detector at
the LHC. The observables studied are the transverse thrust,
thrust minor, and transverse sphericity, each defined using
the final-state charged particles' momentum components
perpendicular to the beam direction. Events with at least
six charged particles are selected by a minimum-bias
trigger. In addition to the differential distributions, the
evolution of each event shape variable as a function of the
leading charged-particle transverse momentum,
charged-particle multiplicity, and summed transverse
momentum is presented. Predictions from several Monte Carlo
models show significant deviations from data. © 2013 CERN.
Published by the American Physical Society.},
Doi = {10.1103/PhysRevD.88.032004},
Key = {fds307586}
}
@article{fds313596,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {Measurement of charged-particle spectra in Pb+Pb collisions
at √sNN = 2.76 TeV with the ATLAS detector at the
LHC},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {9},
Pages = {1-51},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2015)050},
Abstract = {Charged-particle spectra obtained in Pb+Pb interactions at
(Formula presented.) and pp interactions at (Formula
presented.) with the ATLAS detector at the LHC are
presented, using data with integrated luminosities of 0.15
nb−1 and 4.2 pb−1, respectively, in a wide transverse
momentum (0.5 < pT< 150 GeV) and pseudorapidity (|η| < 2)
range. For Pb+Pb collisions, the spectra are presented as a
function of collision centrality, which is determined by the
response of the forward calorimeters located on both sides
of the interaction point. The nuclear modification factors
RAA and RCP are presented in detail as a function of
centrality, pT and η. They show a distinct pT-dependence
with a pronounced minimum at about 7 GeV. Above 60 GeV, RAA
is consistent with a plateau at a centrality-dependent
value, within the uncertainties. The value is 0.55 ±
0.01(stat.) ± 0.04(syst.) in the most central collisions.
The RAA distribution is consistent with flat |η| dependence
over the whole transverse momentum range in all centrality
classes.},
Doi = {10.1007/JHEP09(2015)050},
Key = {fds313596}
}
@article{fds347481,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Coutinho,
YA and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque,
JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas,
AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce,
M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos,
N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and Bylund,
OB and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov,
A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
TM and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati,
L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Gimenez, VC and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen,
H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark,
A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Colasurdo, L and Cole, B and Colijn, AP and Collot, J and Muiño, PC and Coniavitis, E and Connell,
SH},
Title = {Measurement of colour flow using jet-pull observables in t t
¯ events with the ATLAS experiment at s = 13
TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {10},
Pages = {847},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6290-2},
Abstract = {Previous studies have shown that weighted angular moments
derived from jet constituents encode the colour connections
between partons that seed the jets. This paper presents
measurements of two such distributions, the jet-pull angle
and jet-pull magnitude, both of which are derived from the
jet-pull angular moment. The measurement is performed in t t
¯ events with one leptonically decaying <i>W</i> boson and
one hadronically decaying <i>W</i> boson, using 36.1 fb - 1
of <i>pp</i> collision data recorded by the ATLAS detector
at s = 13 TeV delivered by the Large Hadron Collider. The
observables are measured for two dijet systems,
corresponding to the colour-connected daughters of the
<i>W</i> boson and the two <i>b</i>-jets from the top-quark
decays, which are not expected to be colour connected. To
allow the comparison of the measured distributions to colour
model predictions, the measured distributions are unfolded
to particle level, after correcting for experimental effects
introduced by the detector. While good agreement can be
found for some combinations of predictions and observables,
none of the predictions describes the data well across all
observables.},
Doi = {10.1140/epjc/s10052-018-6290-2},
Key = {fds347481}
}
@article{fds316569,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of colour flow with the jet pull angle in tt-
events using the ATLAS detector at √s=8
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {750},
Pages = {475-493},
Publisher = {Elsevier BV},
Year = {2015},
Month = {November},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2015.09.051},
Abstract = {The distribution and orientation of energy inside jets is
predicted to be an experimental handle on colour connections
between the hard-scatter quarks and gluons initiating the
jets. This Letter presents a measurement of the distribution
of one such variable, the jet pull angle. The pull angle is
measured for jets produced in tt- events with one W boson
decaying leptonically and the other decaying to jets using
20.3 fb-1 of data recorded with the ATLAS detector at a
centre-of-mass energy of s=8 TeV at the LHC. The jet pull
angle distribution is corrected for detector resolution and
acceptance effects and is compared to various
models.},
Doi = {10.1016/j.physletb.2015.09.051},
Key = {fds316569}
}
@article{fds307813,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Measurement of CP-violating asymmetries in D0→π
+π - and D0→K +K
- decays at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012009},
Abstract = {We report on a measurement of CP-violating asymmetries (A
CP) in the Cabibbo-suppressed D0→π +π - and D0→K +K -
decays reconstructed in a data sample corresponding to 5.9fb
-1 of integrated luminosity collected by the upgraded
Collider Detector at Fermilab. We use the strong decay D
*+→D0π + to identify the flavor of the charmed meson at
production and exploit CP-conserving strong cc̄ pair
production in pp̄ collisions. High-statistics samples of
Cabibbo-favored D0→K -π + decays with and without a D *±
tag are used to correct for instrumental effects and
significantly reduce systematic uncertainties. We measure A
CP(D0→π +π -)=(+0.22±0.24(stat) ±0.11(syst))% and A
CP(D0→K +K -)=(-0.24±0.22(stat)±0.09(syst))%, in
agreement with CP conservation. These are the most precise
determinations from a single experiment to date. Under the
assumption of negligible direct CP violation in D0→π +π
- and D0→K +K - decays, the results provide an upper limit
to the CP-violating asymmetry in D0 mixing,
|ACPind(D0)|<0.13% at the 90% confidence level. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.012009},
Key = {fds307813}
}
@article{fds307823,
Author = {Aaltonen, T and Ãlvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {Measurement of CP-violation asymmetries in D0→KS0π
+π -},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.032007},
Abstract = {We report a measurement of time-integrated CP-violation
asymmetries in the resonant substructure of the three-body
decay D0→KS0π +π - using CDF II data corresponding to
6.0fb -1 of integrated luminosity from Tevatron pp̄
collisions at √s=1.96TeV. The charm mesons used in this
analysis come from D *+(2010) →D0π + and D *-(2010)→D
̄0π -, where the production flavor of the charm meson is
determined by the charge of the accompanying pion. We apply
a Dalitz-amplitude analysis for the description of the
dynamic decay structure and use two complementary
approaches, namely, a full Dalitz-plot fit employing the
isobar model for the contributing resonances and a
model-independent bin-by-bin comparison of the D0 and D ̄0
Dalitz plots. We find no CP-violation effects and measure an
asymmetry of A CP=(-0.05±0. 57(stat)±0.54(syst))% for the
overall integrated CP-violation asymmetry, consistent with
the standard model prediction. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.032007},
Key = {fds307823}
}
@article{fds307998,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and González, BAL and Amerio,
S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D},
Title = {Measurement of cross sections for b jet production in events
with a Z boson in pp̄ collisions at s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.79.052008},
Abstract = {A measurement of the b jet production cross section is
presented for events containing a Z boson produced in pp̄
collisions at s=1.96TeV, using data corresponding to an
integrated luminosity of 2fb-1 collected by the CDF II
detector at the Tevatron. Z bosons are selected in the
electron and muon decay modes. Jets are considered with
transverse energy ET>20GeV and pseudorapidity |η|<1.5 and
are identified as b jets using a secondary vertex algorithm.
The ratio of the integrated Z+b jet cross section to the
inclusive Z production cross section is measured to be
3.32±0.53(stat)±0.42(syst) ×10-3. This ratio is also
measured differentially in jet ET, jet η, Z-boson
transverse momentum, number of jets, and number of b jets.
The predictions from leading-order Monte Carlo generators
and next-to-leading-order QCD calculations are found to be
consistent with the measurements within experimental and
theoretical uncertainties. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.052008},
Key = {fds307998}
}
@article{fds373544,
Author = {Jackson, P and Kong, AXY and Oliver, JL and Ruggeri, TA and Sharma, AS and White, MJ and Jain, V and Swift, SP and Gingrich, DM and Pinfold, JL and Wang, H and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Cueto, A and Dartsi, O and Delmastro, M and Di Ciaccio,
L and Franco, L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo
Martinez, N and Portales, L and Sauvan, E and Wingerter-Seez, I and Abulaiti, Y and Benjamin, DP and Bhopatkar, VS and Chekanov, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe,
J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Lampl, W and LeBlanc, M and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave,
B and De, K and Eifert, T and Farbin, A and Hadavand, HK and Little, JD and Ozturk, N and Usai, G and White, A and Angelidakis, S and Bellos, P and Fassouliotis, D and Gkialas, I and Kourkoumelis, C and Papageorgiou,
K and Alexopoulos, T and Bakalis, C and Benekos, N and Gazis, EN and Gkountoumis, P and Kitsaki, C and Koulouris, A and Maltezos, S and Paraskevopoulos, C and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Potti, H and Roy, A and Unal,
M and Webb, AF and Beddall, AJ and Celebi, E and Cetin,
SA},
Title = {Measurement of cross sections for production of a Z boson in
association with a flavor-inclusive or doubly b-tagged
large-radius jet in proton-proton collisions at √s = 13
TeV with the ATLAS experiment},
Journal = {Physical Review D},
Volume = {108},
Number = {1},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.108.012022},
Abstract = {We present measurements of cross sections for production of
a leptonically decaying Z boson in association with a
large-radius jet in 13 TeV proton-proton collisions at the
LHC, using 36 fb - 1 of data from the ATLAS detector.
Integrated and differential cross sections are measured at
particle level in both a flavor inclusive and a doubly b
-tagged fiducial phase space. The large-radius jet mass and
transverse momentum, its kinematic relationship to the Z
boson, and the angular separation of b -tagged small-radius
track jets within the large-radius jet are measured. This
measurement constitutes an important test of perturbative
quantum chromodynamics in kinematic and flavor
configurations relevant to several Higgs boson and
beyond-Standard-Model physics analyses. The results
highlight issues with modeling of additional hadronic
activity in the flavor-inclusive selection, and a
distinction between flavor-number schemes in the b -tagged
phase space.},
Doi = {10.1103/PhysRevD.108.012022},
Key = {fds373544}
}
@article{fds307746,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Kesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
G and Arutinov, D},
Title = {Measurement of D *± meson production in jets
from pp collisions at √s=7TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.85.052005},
Abstract = {This paper reports a measurement of D *± meson production
in jets from proton-proton collisions at a center-of-mass
energy of √s=7TeV at the CERN Large Hadron Collider. The
measurement is based on a data sample recorded with the
ATLAS detector with an integrated luminosity of 0.30pb -1
for jets with transverse momentum between 25 and 70 GeV in
the pseudorapidity range |η|<2.5. D *± mesons found in
jets are fully reconstructed in the decay chain: D *+→D0π
+, D0→K -π +, and its charge conjugate. The production
rate is found to be N(D *±)/N(jet)=0.025±0.
001(stat.)±0.004(syst.) for D *± mesons that carry a
fraction z of the jet momentum in the range 0.3<z<1. Monte
Carlo predictions fail to describe the data at small values
of z, and this is most marked at low jet transverse
momentum. © 2012 CERN.},
Doi = {10.1103/PhysRevD.85.052005},
Key = {fds307746}
}
@article{fds315922,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of D⁎±, D± and
Ds± meson production cross sections
in pp collisions at √s=7 TeV with the ATLAS
detector},
Journal = {Nuclear Physics B},
Volume = {907},
Pages = {717-763},
Publisher = {Elsevier BV},
Year = {2016},
Month = {June},
ISSN = {0550-3213},
url = {http://dx.doi.org/10.1016/j.nuclphysb.2016.04.032},
Abstract = {The production of D⁎±, D± and Ds± charmed mesons has
been measured with the ATLAS detector in pp collisions at
s=7 TeV at the LHC, using data corresponding to an
integrated luminosity of 280 nb−1. The charmed mesons have
been reconstructed in the range of transverse momentum
3.5<pT(D)<100 GeV and pseudorapidity |η(D)|<2.1. The
differential cross sections as a function of transverse
momentum and pseudorapidity were measured for D⁎± and D±
production. The next-to-leading-order QCD predictions are
consistent with the data in the visible kinematic region
within the large theoretical uncertainties. Using the
visible D cross sections and an extrapolation to the full
kinematic phase space, the strangeness-suppression factor in
charm fragmentation, the fraction of charged non-strange D
mesons produced in a vector state, and the total cross
section of charm production at s=7 TeV were
derived.},
Doi = {10.1016/j.nuclphysb.2016.04.032},
Key = {fds315922}
}
@article{fds347492,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic,
M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou,
Y},
Title = {Measurement of detector-corrected observables sensitive to
the anomalous production of events with jets and large
missing transverse momentum in p p collisions at s = 13
TeV using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {11},
Pages = {765},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5315-6},
Abstract = {Observables sensitive to the anomalous production of events
containing hadronic jets and missing momentum in the plane
transverse to the proton beams at the Large Hadron Collider
are presented. The observables are defined as a ratio of
cross sections, for events containing jets and large missing
transverse momentum to events containing jets and a pair of
charged leptons from the decay of a Z / γ ∗ boson. This
definition minimises experimental and theoretical systematic
uncertainties in the measurements. This ratio is measured
differentially with respect to a number of kinematic
properties of the hadronic system in two phase-space
regions; one inclusive single-jet region and one region
sensitive to vector-boson-fusion topologies. The data are
found to be in agreement with the Standard Model predictions
and used to constrain a variety of theoretical models for
dark-matter production, including simplified models,
effective field theory models, and invisible decays of the
Higgs boson. The measurements use 3.2 fb - 1 of
proton-proton collision data recorded by the ATLAS
experiment at a centre-of-mass energy of 13 TeV and are
fully corrected for detector effects, meaning that the data
can be used to constrain new-physics models beyond those
shown in this paper.},
Doi = {10.1140/epjc/s10052-017-5315-6},
Key = {fds347492}
}
@article{fds356685,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of differential cross sections and W
+ /W − cross-section ratios for W
boson production in association with jets at √s=8 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {5},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2018)077},
Abstract = {This paper presents a measurement of the W boson production
cross section and the W+/W− cross-section ratio, both in
association with jets, in proton-proton collisions at s=8
TeV with the ATLAS experiment at the Large Hadron Collider.
The measurement is performed in final states containing one
electron and missing transverse momentum using data
corresponding to an integrated luminosity of 20.2 fb−1.
Differential cross sections for events with at least one or
two jets are presented for a range of observables, including
jet transverse momenta and rapidities, the scalar sum of
transverse momenta of the visible particles and the missing
transverse momentum in the event, and the transverse
momentum of the W boson. For a subset of the observables,
the differential cross sections of positively and negatively
charged W bosons are measured separately. In the
cross-section ratio of W+/W− the dominant systematic
uncertainties cancel out, improving the measurement
precision by up to a factor of nine. The observables and
ratios selected for this paper provide valuable input for
the up quark, down quark, and gluon parton distribution
functions of the proton.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP05(2018)077},
Key = {fds356685}
}
@article{fds356542,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Measurement of differential cross sections for single
diffractive dissociation in √s = 8 TeV pp collisions using
the ATLAS ALFA spectrometer},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {2},
Year = {2020},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2020)042},
Abstract = {A dedicated sample of Large Hadron Collider proton-proton
collision data at centre-of-mass energy s = 8 TeV is used to
study inclusive single diffractive dissociation, pp → X p.
The intact final-state proton is reconstructed in the ATLAS
ALFA forward spectrometer, while charged particles from the
dissociated system X are measured in the central detector
components. The fiducial range of the measurement is −4.0
< log10ξ < −1.6 and 0.016 < |t| < 0.43 GeV2, where ξ is
the proton fractional energy loss and t is the squared
four-momentum transfer. The total cross section integrated
across the fiducial range is 1.59 ± 0.13 mb. Cross sections
are also measured differentially as functions of ξ, t, and
∆η, a variable that characterises the rapidity gap
separating the proton and the system X. The data are
consistent with an exponential t dependence, dσ/dt ∝ eBt
with slope parameter B = 7.65 ± 0.34 GeV−2. Interpreted
in the framework of triple Regge phenomenology, the ξ
dependence leads to a pomeron intercept of α(0) = 1.07 ±
0.09. [Figure not available: see fulltext.]},
Doi = {10.1007/JHEP02(2020)042},
Key = {fds356542}
}
@article{fds356700,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of differential cross sections of
isolated-photon plus heavy-flavour jet production in pp
collisions at s=8 TeV using the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {776},
Pages = {295-317},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2017.11.054},
Abstract = {This Letter presents the measurement of differential cross
sections of isolated prompt photons produced in association
with a b-jet or a c-jet. These final states provide
sensitivity to the heavy-flavour content of the proton and
aspects related to the modelling of heavy-flavour quarks in
perturbative QCD. The measurement uses proton–proton
collision data at a centre-of-mass energy of 8 TeV recorded
by the ATLAS detector at the LHC in 2012 corresponding to an
integrated luminosity of up to 20.2 fb−1. The differential
cross sections are measured for each jet flavour with
respect to the transverse energy of the leading photon in
two photon pseudorapidity regions: |ηγ|<1.37 and
1.56<|ηγ|<2.37. The measurement covers photon transverse
energies 25<ETγ<400 GeV and 25<ETγ<350 GeV respectively
for the two |ηγ| regions. For each jet flavour, the ratio
of the cross sections in the two |ηγ| regions is also
measured. The measurement is corrected for detector effects
and compared to leading-order and next-to-leading-order
perturbative QCD calculations, based on various treatments
and assumptions about the heavy-flavour content of the
proton. Overall, the predictions agree well with the
measurement, but some deviations are observed at high photon
transverse energies. The total uncertainty in the
measurement ranges between 13% and 66%, while the central
γ+b measurement exhibits the smallest uncertainty, ranging
from 13% to 27%, which is comparable to the precision of the
theoretical predictions.},
Doi = {10.1016/j.physletb.2017.11.054},
Key = {fds356700}
}
@article{fds347472,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Li, C-Q and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho
Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and CapeansGarrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati,
L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and CastilloGimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
J},
Title = {Measurement of differential cross-sections of a single top
quark produced in association with a W boson at s =
13 TeV with ATLAS.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {3},
Pages = {186},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5649-8},
Abstract = {The differential cross-section for the production of a
<i>W</i> boson in association with a top quark is measured
for several particle-level observables. The measurements are
performed using 36.1 fb - 1 of <i>pp</i> collision data
collected with the ATLAS detector at the LHC in 2015 and
2016. Differential cross-sections are measured in a fiducial
phase space defined by the presence of two charged leptons
and exactly one jet matched to a <i>b</i>-hadron, and are
normalised with the fiducial cross-section. Results are
found to be in good agreement with predictions from several
Monte Carlo event generators.},
Doi = {10.1140/epjc/s10052-018-5649-8},
Key = {fds347472}
}
@article{fds313616,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of differential J/ψ production cross sections
and forward-backward ratios in p + Pb collisions with the
ATLAS detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {October},
ISSN = {0556-2813},
url = {http://dx.doi.org/10.1103/PhysRevC.92.034904},
Abstract = {Measurements of differential cross sections for J/ψ
production in p + Pb collisions at (√SNN at the CERN Large
Hadron Collider with the ATLAS detector are presented. The
data set used corresponds to an integrated luminosity of
28.1 nb−1. The J/ψ mesons are reconstructed in the dimuon
decay channel over the transverse momentum range 8 < pT < 30
GeV and over the center-of-mass rapidity range −2.87 <
y∗ < 1.94. Prompt J/ψ are separated from J/ψ resulting
from b-hadron decays through an analysis of the distance
between the J/ψ decay vertex and the event primary vertex.
The differential cross section for production of nonprompt
J/ψ is compared to a FONLL calculation that does not
include nuclear effects. Forward-backward production ratios
are presented and compared to theoretical predictions. These
results complement previously published results by covering
a region of higher transverse momentum and more central
rapidity. They thus constrain the kinematic dependence of
nuclear modifications of charmonium and b-quark production
in p + Pb collisions.},
Doi = {10.1103/PhysRevC.92.034904},
Key = {fds313616}
}
@article{fds310335,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JJA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of differential production cross sections for Z
/γ∗ bosons in association with jets in p p ¯ collisions
at s =1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.91.012002},
Abstract = {Differential cross sections for the production of Z bosons
or off-shell photons γ∗ in association with jets are
measured in proton-antiproton collisions at center-of-mass
energy s=1.96TeV using the full data set collected with the
Collider Detector at Fermilab in Tevatron run II and
corresponding to 9.6fb-1 of integrated luminosity. Results
include first measurements at CDF of differential cross
sections in events with a Z/γ∗ boson and three or more
jets, the inclusive cross section for production of Z/γ∗
and four or more jets, and cross sections as functions of
various angular observables in lower jet-multiplicity final
states. Measured cross sections are compared to several
theoretical predictions.},
Doi = {10.1103/PhysRevD.91.012002},
Key = {fds310335}
}
@article{fds310356,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of differential production cross-sections for a
Z boson in association with b-jets in 7 TeV proton-proton
collisions with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {10},
Pages = {1-49},
Publisher = {Springer Nature},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2014)141},
Abstract = {Abstract: Measurements of differential production
cross-sections of a Z boson in association with b-jets in pp
collisions at √ = 7 TeV are reported. The data analysed
correspond to an integrated luminosity of 4.6 fb−1
recorded with the ATLAS detector at the Large Hadron
Collider. Particle-level cross-sections are determined for
events with a Z boson decaying into an electron or muon
pair, and containing b-jets. For events with at least one
b-jet, the cross-section is presented as a function of the Z
boson transverse momentum and rapidity, together with the
inclusive b-jet cross-section as a function of b-jet
transverse momentum, rapidity and angular separations
between the b-jet and the Z boson. For events with at least
two b-jets, the cross-section is determined as a function of
the invariant mass and angular separation of the two highest
transverse momentum b-jets, and as a function of the Z boson
transverse momentum and rapidity. Results are compared to
leading-order and next-to-leading-order perturbative QCD
calculations.},
Doi = {10.1007/JHEP10(2014)141},
Key = {fds310356}
}
@booklet{Abbott98o,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G and Fisk, HE and Fisyak, Y and Flattum, E},
Title = {Measurement of dijet angular distributions and search for
quark compositeness},
Journal = {Physical Review Letters},
Volume = {80},
Number = {4},
Pages = {666-671},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.666},
Abstract = {We have measured the dijet angular distribution in s = 1.8
TeV pp collisions using the D0 detector. Order αs3 QCD
predictions are in good agreement with the data. At 95%
confidence limit the data exclude models of quark
compositeness in which the contact interaction scale is
below 2 TeV. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.80.666},
Key = {Abbott98o}
}
@article{fds308132,
Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahmed, SN and Ahn,
SH and Alexeev, GD and Alkhazov, G and Alton, A and Alverson, G and Alves,
GA and Anastasoaie, M and Anderson, S and Andrieu, B and Arnoud, Y and Askew, A and Asman, B and Atramentov, O and Autermann, C and Avila, C and Babukhadia, L and Bacon, TC and Badaud, F and Baden, A and Baffioni, S and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer, P and Barnes, C and Barreto, J and Bartlett, JF and Bassler,
U and Bauer, D and Bean, A and Beauceron, S and Beaudette, F and Begel, M and Bellavance, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram,
I and Besançon, M and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Binder, M and Bischoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Blessing, S and Bloch, D and Blumenschein, U and Boehnlein, A and Boeriu, O and Bolton, TA and Bonamy, P and Borcherding, F and Borissov,
G and Bos, K and Bose, T and Boswell, C and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchanan, NJ and Buchholz,
D and Buehler, M and Buescher, V and Burdin, S and Burnett, TH and Busato,
E and Butler, JM and Bystricky, J and Canelli, F and Carvalho, W and Casey,
BCK and Casey, D and Cason, NM and Castilla-Valdez, H and Chakrabarti,
S and Chakraborty, D and Chan, KM and Chandra, A and Chapin, D and Charles,
F and Cheu, E and Chevalier, L and Cho, DK and Choi, S and Chopra, S and Christiansen, T and Christofek, L and Claes, D and Clark, AR and Clément, B and Clément, C and Coadou, Y and Colling, DJ and Coney, L and Connolly, B and Cooke, M and Cooper, WE and Coppage, D and Corcoran, M and Coss, J and Cothenet, A and Cousinou, M-C and Crépé-Renaudin, S and Cristetiu, M and Cummings, MAC and Cutts, D and da Motta, H and Davies,
B and Davies, G and Davis, GA and De, K and de Jong, P and de Jong, SJ and De
La Cruz-Burelo and E and Martins, CDO and Dean, S and Del Signore and K and Déliot, F and Delsart, PA and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doidge, M and Dong, H and Doulas, S and Duflot, L and Dugad, SR and Duperrin, A and Dyer, J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Eltzroth, JT and Elvira,
VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Fein, D and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisher, W and Fisk, HE and Fleuret, F and Fortner, M and Fox, H and Freeman, W and Fu, S and Fuess, S and Galea, CF and Gallas, E and Galyaev,
E and Gao, M and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gay, P and Gelé, D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Geurkov, G and Ginther, G and Goldmann,
K and Golling, T and Gómez, B and Gounder, K and Goussiou, A and Graham,
G and Grannis, PD and Greder, S and Green, JA and Greenlee, H and Greenwood, ZD and Gregores, EM and Grinstein, S and Gris, P and Grivaz,
J-F and Groer, L and Grünendahl, S and Grünewald, MW and Gu, W and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley,
NJ and Haggerty, H and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki, K and Hanlet, P and Harder, K and Harrington, R and Hauptman, JM and Hauser, R and Hays, C and Hays, J and Hebbeker, T and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper, R and Hou, S and Houben, P and Hu, Y and Huang, J and Huang, Y and Iashvili, I and Illingworth, R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs, K and Jenkins, A and Jesik, R and Jiang, Y and Johns,
K and Johnson, M and Johnson, P and Jonckheere, A and Jonsson, P and Jöstlein, H and Juste, A and Kado, MM and Käfer, D and Kahl, W and Kahn,
S and Kajfasz, E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Ke, Z and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov,
A and Kharchilava, A and Kharzheev, YM and Kim, KH and Klima, B and Klute,
M and Kohli, JM and Kopal, M and Korablev, VM and Kotcher, J and Kothari,
B and Kotwal, AV and Koubarovsky, A and Kouznetsov, O and Kozelov, AV and Kozminski, J and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kurca, T and Kuznetsov, VE and Lager, S and Lahrichi, N and Landsberg,
G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee, SW and Lee,
WM and Leflat, A and Leggett, C and Lehner, F and Leonidopoulos, C and Lewis, P and Li, J and Li, QZ and Li, X and Lima, JGR and Lincoln, D and Linn,
SL and Linnemann, J and Lipaev, VV and Lipton, R and Lobo, L and Lobodenko,
A and Lokajicek, M and Lounis, A and Lu, J and Lubatti, HJ and Lucotte, A and Lueking, L and Luo, C and Lynker, M and Lyon, AL and Maciel, AKA and Madaras, RJ and Mättig, P and Magerkurth, A and Magnan, A-M and Maity,
M and Makovec, N and Mal, PK and Malik, S and Malyshev, VL and Manankov, V and Mao, HS and Maravin, Y and Marshall, T and Martens, M and Martin, MI and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and McMahon, T and Meder, D and Melanson, HL and Melnitchouk, A and Meng, X and Merkin, M and Merritt, KW and Meyer, A and Miao, C and Miettinen, H and Mihalcea, D and Mitrevski, J and Mokhov, N and Molina, J and Mondal, NK and Montgomery, HE and Moore, RW and Mostafa, M and Muanza, GS and Mulders,
M and Mutaf, YD and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding, C and Nomerotski, A and Novaes, SF and Nunnemann, T and Nurse,
E and O'Dell, V and O'Neil, DC and Oguri, V and Oliveira, N and Olivier, B and Oshima, N and Otero y Garzón and GJ and Padley, P and Papageorgiou, K and Parashar, N and Park, J and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Peters, O and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Podesta-Lerma,
PLM and Podstavkov, VM and Pogorelov, Y and Pope, BG and Popkov, E and Prado da Silva and WL and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Quadt, A and Quinn, B and Rani, KJ and Rapidis, PA and Ratoff, PN and Reay, NW and Renardy, J-F and Reucroft,
S and Rha, J and Ridel, M and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Royon, C and Rubinov, P and Ruchti, R and Sabirov,
BM and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro,
A and Savage, G and Sawyer, L and Scanlon, T and Schamberger, RD and Schellman, H and Schieferdecker, P and Schmitt, C and Schukin, AA and Schwartzman, A and Schwienhorst, R and Sengupta, S and Severini, H and Shabalina, E and Shary, V and Shephard, WD and Shpakov, D and Sidwell,
RA and Simak, V and Sirotenko, V and Skow, D and Skubic, P and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Song, Y and Sonnenschein, L and Sopczak, A and Sorín, V and Sosebee, M and Soustruznik, K and Souza, M and Spurlock, B and Stanton, NR and Stark, J and Steele,
J},
Title = {Measurement of dijet azimuthal decorrelations at central
rapidities in pp collisions at sqrt s =1.96
TeV.},
Journal = {Physical review letters},
Volume = {94},
Number = {22},
Pages = {221801},
Year = {2005},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.94.221801},
Abstract = {Correlations in the azimuthal angle between the two largest
transverse momentum jets have been measured using the D0
detector in p (-)p collisions at a center-of-mass energy
sqrt[s]=1.96 TeV. The analysis is based on an inclusive
dijet event sample in the central rapidity region
corresponding to an integrated luminosity of 150 pb(-1).
Azimuthal correlations are stronger at larger transverse
momenta. These are well described in perturbative QCD at
next-to-leading order in the strong coupling constant,
except at large azimuthal differences where contributions
with low transverse momentum are significant.},
Doi = {10.1103/physrevlett.94.221801},
Key = {fds308132}
}
@article{fds356643,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
H},
Title = {Measurement of dijet azimuthal decorrelations in pp
collisions at s =8 TeV with the ATLAS detector and
determination of the strong coupling},
Journal = {Physical Review D},
Volume = {98},
Number = {9},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.98.092004},
Abstract = {A measurement of the rapidity and transverse momentum
dependence of dijet azimuthal decorrelations is presented,
using the quantity RΔφ. The quantity RΔφ specifies the
fraction of the inclusive dijet events in which the
azimuthal opening angle of the two jets with the highest
transverse momenta is less than a given value of the
parameter Δφmax. The quantity RΔφ is measured in
proton-proton collisions at s=8 TeV as a function of the
dijet rapidity interval, the event total scalar transverse
momentum, and Δφmax. The measurement uses an event sample
corresponding to an integrated luminosity of 20.2 fb-1
collected with the ATLAS detector at the CERN Large Hadron
Collider. Predictions of a perturbative QCD calculation at
next-to-leading order in the strong coupling with
corrections for nonperturbative effects are compared to the
data. The theoretical predictions describe the data in the
whole kinematic region. The data are used to determine the
strong coupling αS and to study its running for momentum
transfers from 260 GeV to above 1.6 TeV. Analysis that
combines data at all momentum transfers results in
αS(mZ)=0.1127-0.0027+0.0063.},
Doi = {10.1103/PhysRevD.98.092004},
Key = {fds356643}
}
@article{fds310380,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
JF},
Title = {Measurement of dijet cross-sections in pp collisions at 7
TeV centre-of-mass energy using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {5},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP05(2014)059},
Abstract = {Double-differential dijet cross-sections measured in pp
collisions at the LHC with a 7TeV centre-of-mass energy are
presented as functions of dijet mass and half the rapidity
separation of the two highest-pT jets. These measurements
are obtained using data corresponding to an integrated
luminosity of 4.5 fb−1, recorded by the ATLAS detector in
2011. The data are corrected for detector effects so that
cross-sections are presented at the particle level.
Cross-sections are measured up to 5TeV dijet mass using jets
reconstructed with the anti-kt algorithm for values of the
jet radius parameter of 0.4 and 0.6. The cross-sections are
compared with next-to-leading-order perturbative QCD
calculations by NLOJet++ corrected to account for
non-perturbative effects. Comparisons with POWHEG
predictions, using a next-to-leading-order matrix element
calculation interfaced to a partonshower Monte Carlo
simulation, are also shown. Electroweak effects are
accounted for in both cases. The quantitative comparison of
data and theoretical predictions obtained using various
parameterizations of the parton distribution functions is
performed using a frequentist method. In general, good
agreement with data is observed for the NLOJet++ theoretical
predictions when using the CT10, NNPDF2.1 and MSTW 2008 PDF
sets. Disagreement is observed when using the ABM11 and
HERAPDF1.5 PDF sets for some ranges of dijet mass and half
the rapidity separation. An example setting a lower limit on
the compositeness scale for a model of contact interactions
is presented, showing that the unfolded results can be used
to constrain contributions to dijet production beyond that
predicted by the Standard Model.},
Doi = {10.1007/JHEP05(2014)059},
Key = {fds310380}
}
@article{fds321141,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of dijet production with a veto on additional
central jet activity in pp collisions at √s = 7TeV using
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2011},
Number = {9},
Pages = {1-36},
Publisher = {Springer Nature},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP09(2011)053},
Abstract = {A measurement of jet activity in the rapidity interval
bounded by a dijet system is presented. Events are vetoed if
a jet with transverse momentum greater than 20GeV is found
between the two boundary jets. The fraction of dijet events
that survive the jet veto is presented for boundary jets
that are separated by up to six units of rapidity and with
mean transverse momentum 50 < pT < 500GeV. The mean
multiplicity of jets above the veto scale in the rapidity
interval bounded by the dijet system is also presented as an
alternative method for quantifying perturbative QCD
emission. The data are compared to a next-to-leading order
plus parton shower prediction from the powheg-box, an
all-order resummation using the hej calculation and the
pythia, herwig++ and alpgen event generators. The
measurement was performed using pp collisions at √s = 7TeV
using data recorded by the ATLAS detector in
2010.},
Doi = {10.1007/JHEP09(2011)053},
Key = {fds321141}
}
@article{fds356583,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
Title = {Measurement of distributions sensitive to the underlying
event in inclusive Z boson production in pp collisions at
√s = 13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {8},
Year = {2019},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7162-0},
Abstract = {This paper presents measurements of charged-particle
distributions sensitive to the properties of the underlying
event in events containing a Z boson decaying into a muon
pair. The data were obtained using the ATLAS detector at the
LHC in proton–proton collisions at a centre-of-mass energy
of 13 Te with an integrated luminosity of 3.2fb-1.
Distributions of the charged-particle multiplicity and of
the charged-particle transverse momentum are measured in
regions of the azimuth defined relative to the Z boson
direction. The measured distributions are compared with the
predictions of various Monte Carlo generators which
implement different underyling event models. The Monte Carlo
model predictions qualitatively describe the data well, but
with some significant discrepancies.},
Doi = {10.1140/epjc/s10052-019-7162-0},
Key = {fds356583}
}
@article{fds310388,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Measurement of distributions sensitive to the underlying
event in inclusive Z-boson production in [Formula: see text]
collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {12},
Pages = {3195},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3195-6},
Abstract = {A measurement of charged-particle distributions sensitive to
the properties of the underlying event is presented for an
inclusive sample of events containing a [Formula: see
text]-boson, decaying to an electron or muon pair. The
measurement is based on data collected using the ATLAS
detector at the LHC in proton-proton collisions at a
centre-of-mass energy of [Formula: see text] TeV with an
integrated luminosity of [Formula: see text] fb[Formula:
see text]. Distributions of the charged particle
multiplicity and of the charged particle transverse momentum
are measured in regions of azimuthal angle defined with
respect to the [Formula: see text]-boson direction. The
measured distributions are compared to similar distributions
measured in jet events, and to the predictions of various
Monte Carlo generators implementing different underlying
event models.},
Doi = {10.1140/epjc/s10052-014-3195-6},
Key = {fds310388}
}
@article{fds307923,
Author = {Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, J and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway,
J},
Title = {Measurement of dσ/dy of Drell-Yan e+e-
pairs in the Z mass region from pp̄ collisions at √s=1.96
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {692},
Number = {4},
Pages = {232-239},
Publisher = {Elsevier BV},
Year = {2010},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2010.06.043},
Abstract = {We report on a CDF measurement of the total cross section
and rapidity distribution, dσ/dy, for γ*Z→e+e- events in
the Z boson mass region (66<Mee<116 GeV/c2) produced in pp-
collisions at s=1.96 TeV with 2.1 fb-1 of integrated
luminosity. The measured cross section of 257±16 pb and
dσ/dy distribution are compared with Next-to-Leading-Order
(NLO) and Next-to-Next-to-Leading-Order (NNLO) QCD theory
predictions with CTEQ and MRST/MSTW parton distribution
functions (PDFs). There is good agreement between the
experimental total cross section and dσ/dy measurements
with theoretical calculations with the most recent NNLO
PDFs. © 2010 Elsevier B.V.},
Doi = {10.1016/j.physletb.2010.06.043},
Key = {fds307923}
}
@article{fds307676,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G},
Title = {Measurement of event shapes at large momentum transfer with
the ATLAS detector in pp collisions at √s =7
TeV},
Journal = {European Physical Journal C},
Volume = {72},
Number = {11},
Publisher = {Springer Nature},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2211-y},
Abstract = {A measurement of event shape variables is presented for
large momentum transfer proton-proton collisions using the
ATLAS detector at the Large Hadron Collider. Six event shape
variables calculated using hadronic jets are studied in
inclusive multi-jet events in 35 pb<sup>-1</sup> of
integrated luminosity at a center-of-mass energy of √s = 7
TeV. These measurements are compared to predictions by three
Monte Carlo event generators containing leading-logarithmic
parton showers matched to leading order matrix elements for
2→2 and 2→n (n = 2, …, 6) scattering. Measurements of
the third-jet resolution parameter, aplanarity, thrust,
sphericity, and transverse sphericity are generally well
described. The mean value of each event shape variable is
evaluated as a function of the average momentum of the two
leading jets p<inf>T,1</inf> and p<inf>T,2</inf>, with a
mean pT approaching 1 TeV.},
Doi = {10.1140/epjc/s10052-012-2211-y},
Key = {fds307676}
}
@article{fds307883,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of event shapes in $p\overline{p}$ collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {11},
Pages = {112007},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.112007},
Abstract = {A study of event-shape observables in proton-antiproton
collisions at √s=1.96TeV is presented. The data for this
analysis were recorded by the CDF II Detector at the
Tevatron Collider. The variables studied are the transverse
thrust and thrust minor, both defined in the plane
perpendicular to the beam direction. The observables are
measured using energies from unclustered calorimeter cells.
In addition to studies of the differential distributions, we
present the dependence of event-shape mean values on the
leading-jet transverse energy. Data are compared with pythia
Tune A and to resummed parton-level predictions that were
matched to fixed-order results at next-to-leading-order
(NLO) accuracy (NLO+NLL). Predictions from pythia Tune A
agree fairly well with the data. However, the underlying
event contributes significantly to these observables, making
it difficult to make direct comparisons to the NLO+NLL
predictions, which do not account for the underlying event.
To overcome this difficulty, we introduce a new observable,
a weighted difference of the mean values of the thrust and
thrust minor, which is less sensitive to the underlying
event, allowing for a comparison with NLO+NLL. Both pythia
Tune A and the NLO+NLL calculations agree well within the
20% theoretical uncertainty with the data for this
observable, indicating that perturbative QCD successfully
describes shapes of the hadronic final states. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.112007},
Key = {fds307883}
}
@article{fds310369,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O and Arnal, V},
Title = {Measurement of event-plane correlations in √sNN
= 2.76 TeV lead-lead collisions with the ATLAS
detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {90},
Number = {2},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevC.90.024905},
Abstract = {A measurement of event-plane correlations involving two or
three event planes of different order is presented as a
function of centrality for 7 μb-1 Pb+Pb collision data at
sNN=2.76 TeV, recorded by the ATLAS experiment at the Large
Hadron Collider. Fourteen correlators are measured using a
standard event-plane method and a scalar-product method, and
the latter method is found to give a systematically larger
correlation signal. Several different trends in the
centrality dependence of these correlators are observed.
These trends are not reproduced by predictions based on the
Glauber model, which includes only the correlations from the
collision geometry in the initial state. Calculations that
include the final-state collective dynamics are able to
describe qualitatively, and in some cases also
quantitatively, the centrality dependence of the measured
correlators. These observations suggest that both the
fluctuations in the initial geometry and the nonlinear
mixing between different harmonics in the final state are
important for creating these correlations in momentum
space.},
Doi = {10.1103/PhysRevC.90.024905},
Key = {fds310369}
}
@article{fds321116,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
Title = {Measurement of event-shape observables in [Formula: see
text] events in pp collisions at [Formula: see
text] [Formula: see text] with the ATLAS detector at the
LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {7},
Pages = {375},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4176-8},
Abstract = {Event-shape observables measured using charged particles in
inclusive <i>Z</i>-boson events are presented, using the
electron and muon decay modes of the <i>Z</i> bosons. The
measurements are based on an integrated luminosity of
[Formula: see text] of proton-proton collisions recorded by
the ATLAS detector at the LHC at a centre-of-mass energy
[Formula: see text] [Formula: see text]. Charged-particle
distributions, excluding the lepton-antilepton pair from the
<i>Z</i>-boson decay, are measured in different ranges of
transverse momentum of the <i>Z</i> boson. Distributions
include multiplicity, scalar sum of transverse momenta, beam
thrust, transverse thrust, spherocity, and [Formula: see
text]-parameter, which are in particular sensitive to
properties of the underlying event at small values of the
<i>Z</i>-boson transverse momentum. The measured observables
are compared with predictions from Pythia 8, Sherpa, and
Herwig 7. Typically, all three Monte Carlo generators
provide predictions that are in better agreement with the
data at high <i>Z</i>-boson transverse momenta than at low
<i>Z</i>-boson transverse momenta, and for the observables
that are less sensitive to the number of charged particles
in the event.},
Doi = {10.1140/epjc/s10052-016-4176-8},
Key = {fds321116}
}
@article{fds371907,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Measurement of exclusive pion pair production in
proton–proton collisions at √s=7TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11700-x},
Abstract = {The exclusive production of pion pairs in the process pp→
ppπ+π- has been measured at s=7TeV with the ATLAS detector
at the LHC, using 80μb-1 of low-luminosity data. The pion
pairs were detected in the ATLAS central detector while
outgoing protons were measured in the forward ATLAS ALFA
detector system. This represents the first use of proton
tagging to measure an exclusive hadronic final state at the
LHC. A cross-section measurement is performed in two
kinematic regions defined by the proton momenta, the pion
rapidities and transverse momenta, and the pion–pion
invariant mass. Cross-section values of 4.8±1.0(stat)-0.2+0.3(syst)μb
and 9±6(stat)-2+2(syst)μb are obtained in the two regions;
they are compared with theoretical models and provide a
demonstration of the feasibility of measurements of this
type.},
Doi = {10.1140/epjc/s10052-023-11700-x},
Key = {fds371907}
}
@article{fds321114,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of exclusive γγ →w+W- production and search
for exclusive Higgs boson production in pp collisions at s
=8 TeV using the ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032011},
Abstract = {Searches for exclusively produced W boson pairs in the
process pp(γγ)→pW+W-p and an exclusively produced Higgs
boson in the process pp(gg)→pHp have been performed using
e±μ final states. These measurements use 20.2 fb-1 of pp
collisions collected by the ATLAS experiment at a
center-of-mass energy s=8 TeV at the LHC. Exclusive
production of W+W- consistent with the Standard Model
prediction is found with 3.0σ significance. The exclusive
W+W- production cross section is determined to be
σ(γγ→W+W-→e±μX)=6.9±2.2(stat)±1.4(sys) fb, in
agreement with the Standard Model prediction. Limits on
anomalous quartic gauge couplings are set at 95% confidence
level as -1.7×10-6<a0W/Λ2<1.7×10-6 GeV-2 and
-6.4×10-6<aCW/Λ2<6.3×10-6 GeV-2. A 95% confidence-level
upper limit on the total production cross section for an
exclusive Higgs boson is set to 1.2 pb.},
Doi = {10.1103/PhysRevD.94.032011},
Key = {fds321114}
}
@article{fds310259,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of exclusive γγ→ℓ+ℓ−
production in proton–proton collisions at √s=7 TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {749},
Pages = {242-261},
Publisher = {Elsevier BV},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2015.07.069},
Abstract = {This Letter reports a measurement of the exclusive
γγ→ℓ+ℓ− (ℓ=e, μ) cross-section in
proton–proton collisions at a centre-of-mass energy of 7
TeV by the ATLAS experiment at the LHC, based on an
integrated luminosity of 4.6 fb−1. For the electron or
muon pairs satisfying exclusive selection criteria, a fit to
the dilepton acoplanarity distribution is used to extract
the fiducial cross-sections. The cross-section in the
electron channel is determined to be σγγ→e+e−excl.=0.428
± 0.035 (stat.) ± 0.018 (syst.) pb for a phase–space
region with invariant mass of the electron pairs greater
than 24 GeV, in which both electrons have transverse
momentum pT>12 GeV and pseudorapidity |η|<2.4. For muon
pairs with invariant mass greater than 20 GeV, muon
transverse momentum pT>10 GeV and pseudorapidity |η|<2.4,
the cross-section is determined to be σγγ→μ+μ−excl.=0.628
± 0.032 (stat.) ± 0.021 (syst.) pb. When proton absorptive
effects due to the finite size of the proton are taken into
account in the theory calculation, the measured
cross-sections are found to be consistent with the theory
prediction.},
Doi = {10.1016/j.physletb.2015.07.069},
Key = {fds310259}
}
@article{fds356568,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud,
AA and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob,
M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G},
Title = {Measurement of fiducial and differential
W+W- production cross-sections at
√s=13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {10},
Year = {2019},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7371-6},
Abstract = {A measurement of fiducial and differential cross-sections
for W+W- production in proton–proton collisions at
s=13 TeV with the ATLAS experiment at the Large Hadron
Collider using data corresponding to an integrated
luminosity of 36.1 fb - 1 is presented. Events with one
electron and one muon are selected, corresponding to the
decay of the diboson system as WW→ e±νμ∓ν. To
suppress top-quark background, events containing jets with a
transverse momentum exceeding 35 GeV are not included in
the measurement phase space. The fiducial cross-section, six
differential distributions and the cross-section as a
function of the jet-veto transverse momentum threshold are
measured and compared with several theoretical predictions.
Constraints on anomalous electroweak gauge boson
self-interactions are also presented in the framework of a
dimension-six effective field theory.},
Doi = {10.1140/epjc/s10052-019-7371-6},
Key = {fds356568}
}
@article{fds321107,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Measurement of fiducial differential cross sections of
gluon-fusion production of Higgs bosons decaying to WW
∗→eνμν with the ATLAS detector at √s=8
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)104},
Abstract = {This paper describes a measurement of fiducial and
differential cross sections of gluon-fusion Higgs boson
production in the H → W W∗→ eνμν channel, using
20.3 fb−1 of proton-proton collision data. The data were
produced at a centre-of-mass energy of s=8 TeV at the CERN
Large Hadron Collider and recorded by the ATLAS detector in
2012. Cross sections are measured from the observed H→ W
W∗→ eνμν signal yield in categories distinguished by
the number of associated jets. The total cross section is
measured in a fiducial region defined by the kinematic
properties of the charged leptons and neutrinos.
Differential cross sections are reported as a function of
the number of jets, the Higgs boson transverse momentum, the
dilepton rapidity, and the transverse momentum of the
leading jet. The jet-veto efficiency, or fraction of events
with no jets above a given transverse momentum threshold, is
also reported. All measurements are compared to QCD
predictions from Monte Carlo generators and fixed-order
calculations, and are in agreement with the Standard Model
predictions.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP08(2016)104},
Key = {fds321107}
}
@article{fds356555,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Measurement of flow harmonics correlations with mean
transverse momentum in lead–lead and proton–lead
collisions at √sNN=5.02TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {12},
Year = {2019},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7489-6},
Abstract = {To assess the properties of the quark–gluon plasma formed
in ultrarelativistic ion collisions, the ATLAS experiment at
the LHC measures a correlation between the mean transverse
momentum and the flow harmonics. The analysis uses data
samples of lead–lead and proton–lead collisions obtained
at the centre-of-mass energy per nucleon pair of 5.02 TeV,
corresponding to total integrated luminosities of 22μb-1
and 28nb-1, respectively. The measurement is performed using
a modified Pearson correlation coefficient with the
charged-particle tracks on an event-by-event basis. The
modified Pearson correlation coefficients for the 2nd-,
3rd-, and 4th-order flow harmonics are measured in the
lead–lead collisions as a function of event centrality
quantified as the number of charged particles or the number
of nucleons participating in the collision. The measurements
are performed for several intervals of the charged-particle
transverse momentum. The correlation coefficients for all
studied harmonics exhibit a strong centrality evolution,
which only weakly depends on the charged-particle momentum
range. In the proton–lead collisions, the modified Pearson
correlation coefficient measured for the 2nd-order flow
harmonics shows only weak centrality dependence. The
lead-lead data is qualitatively described by the predictions
based on the hydrodynamical model.},
Doi = {10.1140/epjc/s10052-019-7489-6},
Key = {fds356555}
}
@article{fds313588,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Measurement of flow harmonics with multi-particle cumulants
in Pb+Pb collisions at [Formula: see text] TeV with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {11},
Pages = {3157},
Year = {2014},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3157-z},
Abstract = {ATLAS measurements of the azimuthal anisotropy in lead-lead
collisions at [Formula: see text] TeV are shown using a
dataset of approximately 7 [Formula: see text]b[Formula:
see text] collected at the LHC in 2010. The measurements are
performed for charged particles with transverse momenta
[Formula: see text] GeV and in the pseudorapidity range
[Formula: see text]. The anisotropy is characterized by the
Fourier coefficients, [Formula: see text], of the
charged-particle azimuthal angle distribution for [Formula:
see text]-4. The Fourier coefficients are evaluated using
multi-particle cumulants calculated with the generating
function method. Results on the transverse momentum,
pseudorapidity and centrality dependence of the [Formula:
see text] coefficients are presented. The elliptic flow,
[Formula: see text], is obtained from the two-, four-, six-
and eight-particle cumulants while higher-order
coefficients, [Formula: see text] and [Formula: see text],
are determined with two- and four-particle cumulants. Flow
harmonics [Formula: see text] measured with four-particle
cumulants are significantly reduced compared to the
measurement involving two-particle cumulants. A comparison
to [Formula: see text] measurements obtained using different
analysis methods and previously reported by the LHC
experiments is also shown. Results of measurements of flow
fluctuations evaluated with multi-particle cumulants are
shown as a function of transverse momentum and the collision
centrality. Models of the initial spatial geometry and its
fluctuations fail to describe the flow fluctuations
measurements.},
Doi = {10.1140/epjc/s10052-014-3157-z},
Key = {fds313588}
}
@article{fds356749,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of forward-backward multiplicity correlations in
lead-lead, proton-lead, and proton-proton collisions with
the ATLAS detector},
Journal = {Physical Review C},
Volume = {95},
Number = {6},
Year = {2017},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevC.95.064914},
Abstract = {Two-particle pseudorapidity correlations are measured in
sNN=2.76TeVPb+Pb, sNN=5.02TeVp+Pb, and s=13TeVpp collisions
at the Large Hadron Collider (LHC), with total integrated
luminosities of approximately 7μb-1, 28 nb-1, and 65 nb-1,
respectively. The correlation function CN(η1,η2) is
measured as a function of event multiplicity using charged
particles in the pseudorapidity range |η|<2.4. The
correlation function contains a significant short-range
component, which is estimated and subtracted. After removal
of the short-range component, the shape of the correlation
function is described approximately by 1+(a12)1/2η1η2 in
all collision systems over the full multiplicity range. The
values of (a12)1/2 are consistent for the opposite-charge
pairs and same-charge pairs, and for the three collision
systems at similar multiplicity. The values of (a12)1/2 and
the magnitude of the short-range component both follow a
power-law dependence on the event multiplicity. The
short-range component in p + Pb collisions, after
symmetrizing the proton and lead directions, is found to be
smaller at a given η than in pp collisions with comparable
multiplicity.},
Doi = {10.1103/PhysRevC.95.064914},
Key = {fds356749}
}
@article{fds313615,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of four-jet differential cross sections in
√s=8 TeV proton-proton collisions using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {12},
Pages = {1-76},
Publisher = {Springer Nature},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2015)105},
Abstract = {Differential cross sections for the production of at least
four jets have been measured in proton-proton collisions at
(Formula presented.) TeV at the Large Hadron Collider using
the ATLAS detector. Events are selected if the four anti-ktR
= 0.4 jets with the largest transverse momentum (pT) within
the rapidity range |y| < 2.8 are well separated (ΔR4jmin >
0.65), all have pT > 64 GeV, and include at least one jet
with pT > 100 GeV. The dataset corresponds to an integrated
luminosity of 20.3 fb−1. The cross sections, corrected for
detector effects, are compared to leading-order and
next-to-leading-order calculations as a function of the jet
momenta, invariant masses, minimum and maximum opening
angles and other kinematic variables.},
Doi = {10.1007/JHEP12(2015)105},
Key = {fds313615}
}
@article{fds355146,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Measurement of hadronic event shapes in high-p T
multijet final states at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {1},
Year = {2021},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2021)188},
Abstract = {A measurement of event-shape variables in proton-proton
collisions at large momentum transfer is presented using
data collected at s = 13 TeV with the ATLAS detector at the
Large Hadron Collider. Six event-shape variables calculated
using hadronic jets are studied in inclusive multijet events
using data corresponding to an integrated luminosity of 139
fb−1. Measurements are performed in bins of jet
multiplicity and in different ranges of the scalar sum of
the transverse momenta of the two leading jets, reaching
scales beyond 2 TeV. These measurements are compared with
predictions from Monte Carlo event generators containing
leading-order or next-to-leading order matrix elements
matched to parton showers simulated to leading-logarithm
accuracy. At low jet multiplicities, shape discrepancies
between the measurements and the Monte Carlo predictions are
observed. At high jet multiplicities, the shapes are better
described but discrepancies in the normalisation are
observed. [Figure not available: see fulltext.]},
Doi = {10.1007/JHEP01(2021)188},
Key = {fds355146}
}
@article{fds317295,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Ochoa, MI and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurement of hard double-parton interactions in W(→ lν)
+ 2-jet events at √s = 7 TeV with the ATLAS
detector},
Journal = {New Journal of Physics},
Volume = {15},
Number = {3},
Pages = {033038-033038},
Publisher = {IOP Publishing},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1088/1367-2630/15/3/033038},
Abstract = {The production of W bosons in association with two jets in
proton-proton collisions at a centre-of-mass energy of √ s
= 7 TeV has been analysed for the presence of double-parton
interactions using data corresponding to an integrated
luminosity of 36 pb-1, collected with the ATLAS detector at
the Large Hadron Collider. The fraction of events arising
from double-parton interactions, f(D)DP, has been measured
through the pT balance between the two jets and amounts to
f(D)DP = 0.08 ±0.01 (stat.)±0.02 (sys.) for jets with
transverse momentum pT > 20 GeV and rapidity |y| < 2.8. This
corresponds to a measurement of the effective area parameter
for hard double-parton interactions of σeff = 15 ± 3
(stat.) +5-3 (sys.) mb.},
Doi = {10.1088/1367-2630/15/3/033038},
Key = {fds317295}
}
@article{fds310340,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Measurement of Higgs boson production in the diphoton decay
channel in pp collisions at center-of-mass energies of 7 and
8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.112015},
Abstract = {A measurement of the production processes of the recently
discovered Higgs boson is performed in the two-photon final
state using 4.5 fb-1of proton-proton collisions data at √s
= 7 TeV and 20.3 fb-1at √s = 8 TeV collected by the ATLAS
detector at the Large Hadron Collider. The number of
observed Higgs boson decays to diphotons divided by the
corresponding Standard Model prediction, called the signal
strength, is found to be μ = 1.17 ± 0.27 at the value of
the Higgs boson mass measured by ATLAS, mH= 125.4 GeV. The
analysis is optimized to measure the signal strengths for
individual Higgs boson production processes at this value of
mH. They are found to be μggF= 1.32 ± 0.38, μVBF= 0.8 ±
0.7, μWH= 1.0 ± 1.6, μZH= 0.1+3.7-0.1, and μtt¯H=
1.6+2.7-1.8, for Higgs boson production through gluon
fusion, vector-boson fusion, and in association with a W or
Z boson or a top-quark pair, respectively. Compared with the
previously published ATLAS analysis, the results reported
here also benefit from a new energy calibration procedure
for photons and the subsequent reduction of the systematic
uncertainty on the diphoton mass resolution. No significant
deviations from the predictions of the Standard Model are
found.},
Doi = {10.1103/PhysRevD.90.112015},
Key = {fds310340}
}
@article{fds329966,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurement of inclusive and differential cross sections in
the H → ZZ * → 4ℓ decay channel in pp
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {10},
Publisher = {Springer Nature},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2017)132},
Abstract = {Inclusive and differential fiducial cross sections of Higgs
boson production in proton-proton collisions are measured in
the H → ZZ* → 4ℓ decay channel. The proton-proton
collision data were produced at the Large Hadron Collider at
a centre-of-mass energy of 13 TeV and recorded by the ATLAS
detector in 2015 and 2016, corresponding to an integrated
luminosity of 36.1 fb−1. The inclusive fiducial cross
section in the H → ZZ* → 4ℓ decay channel is measured
to be 3.62 ± 0.50(stat)− 0.20+ 0.25 (sys) fb, in
agreement with the Standard Model prediction of 2.91 ± 0.13
fb. The cross section is also extrapolated to the total
phase space including all Standard Model Higgs boson decays.
Several differential fiducial cross sections are measured
for observables sensitive to the Higgs boson production and
decay, including kinematic distributions of jets produced in
association with the Higgs boson. Good agreement is found
between data and Standard Model predictions. The results are
used to put constraints on anomalous Higgs boson
interactions with Standard Model particles, using the
pseudo-observable extension to the kappa-framework.[Figure
not available: see fulltext.].},
Doi = {10.1007/JHEP10(2017)132},
Key = {fds329966}
}
@article{fds308138,
Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahn, SH and Ahsan, M and Alexeev,
GD and Alkhazov, G and Alton, A and Alverson, G and Alves, GA and Anastasoaie, M and Andeen, T and Anderson, S and Andrieu, B and Arnoud,
Y and Askew, A and Asman, B and Assis Jesus and ACS and Atramentov, O and Autermann, C and Avila, C and Badaud, F and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer,
P and Barnes, C and Barreto, J and Bartlett, JF and Bassler, U and Bauer,
D and Bean, A and Beauceron, S and Begel, M and Bellavance, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Binder,
M and Biscarat, C and Black, KM and Blackler, I and Blazey, G and Blekman,
F and Blessing, S and Bloch, D and Blumenschein, U and Boehnlein, A and Boeriu, O and Bolton, TA and Borcherding, F and Borissov, G and Bos, K and Bose, T and Brandt, A and Brock, R and Brooijmans, G and Bross, A and Buchanan, NJ and Buchholz, D and Buehler, M and Buescher, V and Burdin,
S and Burnett, TH and Busato, E and Butler, JM and Bystricky, J and Caron,
S and Carvalho, W and Casey, BCK and Cason, NM and Castilla-Valdez, H and Chakrabarti, S and Chakraborty, D and Chan, KM and Chandra, A and Chapin, D and Charles, F and Cheu, E and Cho, DK and Choi, S and Choudhary,
B and Christiansen, T and Christofek, L and Claes, D and Clément, B and Clément, C and Coadou, Y and Cooke, M and Cooper, WE and Coppage, D and Corcoran, M and Cothenet, A and Cousinou, M-C and Cox, B and Crépé-Renaudin, S and Cristetiu, M and Cutts, D and da Motta, H and Davies, B and Davies, G and Davis, GA and De, K and de Jong, P and de Jong,
SJ and De La Cruz-Burelo and E and De Oliveira Martins and C and Dean, S and Degenhardt, JD and Déliot, F and Demarteau, M and Demina, R and Demine,
P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg,
M and Doidge, M and Dong, H and Doulas, S and Dudko, LV and Duflot, L and Dugad, SR and Duperrin, A and Dyer, J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Elvira,
VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisher, W and Fisk, HE and Fleck, I and Fortner, M and Fox, H and Fu, S and Fuess, S and Gadfort, T and Galea, CF and Gallas, E and Galyaev, E and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gay, P and Gelé,
D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Ginther,
G and Golling, T and Gómez, B and Gounder, K and Goussiou, A and Grannis,
PD and Greder, S and Greenlee, H and Greenwood, ZD and Gregores, EM and Gris, P and Grivaz, J-F and Groer, L and Grünendahl, S and Grünewald,
MW and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley, NJ and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki, K and Harder, K and Harrington, R and Hauptman, JM and Hauser,
R and Hays, J and Hebbeker, T and Hedin, D and Heinmiller, JM and Heinson,
AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky,
R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper,
R and Houben, P and Hu, Y and Huang, J and Iashvili, I and Illingworth, R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs, K and Jenkins, A and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jonsson, P and Juste, A and Käfer, D and Kahl, W and Kahn, S and Kajfasz,
E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Kaur, R and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov, A and Kharchilava, A and Kharzheev, YM and Kim, H and Klima, B and Klute, M and Kohli, JM and Kopal, M and Korablev, VM and Kotcher, J and Kothari, B and Koubarovsky, A and Kozelov, AV and Kozminski, J and Kryemadhi, A and Krzywdzinski, S and Kuleshov, S and Kulik, Y and Kumar, A and Kunori, S and Kupco, A and Kurca, T and Kvita, J and Lager, S and Lahrichi, N and Landsberg, G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee,
WM and Leflat, A and Lehner, F and Leonidopoulos, C and Leveque, J and Lewis, P and Li, J and Li, QZ and Lima, JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipaev, VV and Lipton, R and Lobo, L and Lobodenko, A and Lokajicek, M and Lounis, A and Love, P and Lubatti, HJ and Lueking, L and Lynker, M and Lyon, AL and Maciel, AKA and Madaras, RJ and Mättig, P and Magass, C and Magerkurth, A and Magnan, A-M and Makovec, N and Mal, PK and Malbouisson, HB and Malik, S and Malyshev, VL and Mao, HS and Maravin,
Y and Martens, M and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and Meder, D and Melanson, HL and Melnitchouk, A and Mendes, A and Merkin, M and Merritt, KW and Meyer, A and Michaut, M and Miettinen, H and Mitrevski, J and Mokhov, N and Molina, J and Mondal,
NK and Moore, RW and Muanza, GS and Mulders, M and Mutaf, YD and Nagy, E and Narain, M and Naumann, NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding, C and Nomerotski, A and Novaes, SF and Nunnemann, T and Nurse, E and O'Dell, V and O'Neil, DC and Oguri, V and Oliveira, N and Oshima, N and Otero y Garzón and GJ and Padley, P and Parashar, N and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Pleier, M-A and Podesta-Lerma, PLM and Podstavkov, VM and Pogorelov, Y and Pope, BG and Silva, WLPD and Prosper, HB and Protopopescu, S and Qian, J and Quadt, A and Quinn, B and Rani, KJ and Ranjan, K and Rapidis, PA and Ratoff, PN and Reay, NW and Reucroft, S and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Rodrigues, RF and Royon, C and Rubinov, P and Ruchti, R and Rud, VI and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro, A and Savage, G and Sawyer, L and Scanlon, T and Schaile, D and Schamberger,
RD and Schellman, H and Schieferdecker, P and Schmitt, C and Schwartzman, A and Schwienhorst, R and Sengupta, S and Severini, H and Shabalina, E and Shamim, M and Shary, V and Shchukin, AA and Shephard,
WD and Shivpuri, RK and Shpakov, D and Sidwell, RA and Simak, V and Sirotenko, V and Skubic, P and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Sonnenschein, L and Sopczak, A and Sosebee, M and Soustruznik, K and Souza, M and Spurlock, B and Stanton, NR and Stark, J and Steele, J and Stevenson, K and Stolin, V and Stone, A and Stoyanova, DA and Strandberg, J and Strang, MA and Strauss, M and Ströhmer, R and Strom,
D and Strovink, M and Stutte, L and Sumowidagdo, S and Sznajder, A and Talby, M and Tamburello, P and Taylor, W and Telford, P and Temple, J and Thomas, E and Thooris, B and Tomoto, M and Toole, T and Torborg, J and Towers, S and Trefzger, T and Trincaz-Duvoid, S and Tuchming, B and Tully, C and Turcot, AS and Tuts, PM and Uvarov, L and Uvarov, S and Uzunyan, S and Vachon, B and Van Kooten and R and van Leeuwen, WM and Varelas, N and Varnes, EW and Vartapetian, A and Vasilyev, IA and Vaupel, M and Verdier, P and Vertogradov, LS and Verzocchi, M and Villeneuve-Seguier, F and Vlimant, J-R and Von Toerne and E and Vreeswijk, M and Vu, AT and Wahl, HD and Walker, R and Wang, L and Wang,
Z-M and Warchol, J and Watts, G},
Title = {Measurement of inclusive differential cross sections for pp
collisions at (square root)s = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {94},
Number = {23},
Pages = {232001},
Year = {2005},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.94.232001},
Abstract = {We present measurements of the inclusive production cross
sections of the Gamma(1S) bottomonium state in pp collisions
at (square root)s = 1.96 TeV. Using the Gamma(1S) -->
mu(+)mu(-) decay mode for a data sample of 159 +/- 10 pb(-1)
collected by the D0 detector at the Fermilab Tevatron
collider, we determine the differential cross sections as a
function of the Gamma(1S) transverse momentum for three
ranges of the Gamma(1S) rapidity: 0 < y(Gamma) < or = 0.6,
0.6 < y(Gamma) < or = 1.2, and 1.2 < y(Gamma) < or =
1.8.},
Doi = {10.1103/physrevlett.94.232001},
Key = {fds308138}
}
@article{fds356686,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of inclusive jet and dijet cross-sections in
proton-proton collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {5},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2018)195},
Abstract = {Inclusive jet and dijet cross-sections are measured in
proton-proton collisions at a centre-of-mass energy of 13
TeV. The measurement uses a dataset with an integrated
luminosity of 3.2 fb−1 recorded in 2015 with the ATLAS
detector at the Large Hadron Collider. Jets are identified
using the anti-kt algorithm with a radius parameter value of
R = 0.4. The inclusive jet cross-sections are measured
double-differentially as a function of the jet transverse
momentum, covering the range from 100 GeV to 3.5 TeV, and
the absolute jet rapidity up to |y| = 3. The
double-differential dijet production cross-sections are
presented as a function of the dijet mass, covering the
range from 300 GeV to 9 TeV, and the half absolute rapidity
separation between the two leading jets within |y| < 3,
y∗, up to y∗ = 3. Next-to-leading-order, and
next-to-next-to-leading-order for the inclusive jet
measurement, perturbative QCD calculations corrected for
non-perturbative and electroweak effects are compared to the
measured cross-sections.},
Doi = {10.1007/JHEP05(2018)195},
Key = {fds356686}
}
@article{fds307747,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A},
Title = {Measurement of inclusive jet and dijet production in pp
collisions at √s=7TeV using the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.86.014022},
Abstract = {Inclusive jet and dijet cross sections have been measured in
proton-proton collisions at a center-of-mass energy of 7 TeV
using the ATLAS detector at the Large Hadron Collider. The
cross sections were measured using jets clustered with the
anti-kt algorithm with parameters R=0.4 and R=0.6. These
measurements are based on the 2010 data sample, consisting
of a total integrated luminosity of 37pb-1. Inclusive jet
double-differential cross sections are presented as a
function of jet transverse momentum, in bins of jet
rapidity. Dijet double-differential cross sections are
studied as a function of the dijet invariant mass, in bins
of half the rapidity separation of the two leading jets. The
measurements are performed in the jet rapidity range
|y|<4.4, covering jet transverse momenta from 20 GeV to 1.5
TeV and dijet invariant masses from 70 GeV to 5 TeV. The
data are compared to expectations based on
next-to-leading-order QCD calculations corrected for
nonperturbative effects, as well as to next-to-leading-order
Monte Carlo predictions. In addition to a test of the theory
in a new kinematic regime, the data also provide sensitivity
to parton distribution functions in a region where they are
currently not well-constrained. © 2012 CERN. Published by
the American Physical Society under the terms of the
http://creativecommons.org/licenses/by/ 3.0/ Creative
Commons Attribution 3.0 License. Further distribution of
this work must maintain attribution to the author(s) and the
published article's title, journal citation, and
DOI.},
Doi = {10.1103/PhysRevD.86.014022},
Key = {fds307747}
}
@article{fds313587,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of inclusive jet charged-particle fragmentation
functions in Pb+Pb collisions at √sNN=2.76 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {739},
Pages = {320-342},
Publisher = {Elsevier BV},
Year = {2014},
Month = {December},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2014.10.065},
Abstract = {Measurements of charged-particle fragmentation functions of
jets produced in ultra-relativistic nuclear collisions can
provide insight into the modification of parton showers in
the hot, dense medium created in the collisions. ATLAS has
measured jets in sNN=2.76 TeV Pb+Pb collisions at the LHC
using a data set recorded in 2011 with an integrated
luminosity of 0.14 nb−1. Jets were reconstructed using the
anti-kt algorithm with distance parameter values
R=0.2,0.3,and 0.4. Distributions of charged-particle
transverse momentum and longitudinal momentum fraction are
reported for seven bins in collision centrality for R=0.4
jets with pTjet>100 GeV. Commensurate minimum pT values are
used for the other radii. Ratios of fragment distributions
in each centrality bin to those measured in the most
peripheral bin are presented. These ratios show a reduction
of fragment yield in central collisions relative to
peripheral collisions at intermediate z values,
0.04≲z≲0.2, and an enhancement in fragment yield for
z≲0.04. A smaller, less significant enhancement is
observed at large z and large pT in central
collisions.},
Doi = {10.1016/j.physletb.2014.10.065},
Key = {fds313587}
}
@article{fds310406,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of inclusive two-particle angular correlations
in pp collisions with the atlas detector at the
LHC},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {5},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP05(2012)157},
Abstract = {We present a measurement of two-particle angular
correlations in protonproton collisions at √a = 900 GeV
and 7TeV. The collision events were collected during 2009
and 2010 with the ATLAS detector at the Large Hadron
Collider using a single-arm minimum bias trigger.
Correlations are measured for charged particles produced in
the kinematic range of transverse momentum pT > 100MeV and
pseudorapidity |n| < 2.5. A complex structure in
pseudorapidity and azimuth is observed at both collision
energies. Results are compared to pythia 8 and herwig++ as
well as to the AMBT2B, DW and Perugia 2011 tunes of pythia
6. The data are not satisfactorily described by any of these
models.},
Doi = {10.1007/JHEP05(2012)157},
Key = {fds310406}
}
@article{fds310341,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of indirect CP -violating asymmetries in D0
→k+K- and D0 →π+π- decays at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.111103},
Abstract = {We report a measurement of the indirect CP-violating
asymmetries (AΓ) between effective lifetimes of anticharm
and charm mesons reconstructed in D0→K+K- and D0→π+π-
decays. We use the full data set of proton-antiproton
collisions collected by the Collider Detector at Fermilab
experiment and corresponding to 9.7fb-1 of integrated
luminosity. The strong-interaction decay D∗+→D0π+ is
used to identify the meson at production as D0 or D¯0. We
statistically subtract D0 and D¯0 mesons originating from
b-hadron decays and measure the yield asymmetry between
anticharm and charm decays as a function of decay time. We
measure AΓ(K+K-)=(-0.19±0.15(stat)±0.04(syst))% and
AΓ(π+π-)=(-0.01±0.18(stat)±0.03(syst))%. The results
are consistent with the hypothesis of CP symmetry and their
combination yields AΓ=(-0.12±0.12)%.},
Doi = {10.1103/PhysRevD.90.111103},
Key = {fds310341}
}
@article{fds307645,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurement of isolated-photon pair production in pp
collisions at √s=7TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {1},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2013)086},
Abstract = {The ATLAS experiment at the LHC has measured the production
cross section of events with two isolated photons in the
final state, in proton-proton collisions at √s=7TeV . The
full data set collected in 2011, corresponding to an
integrated luminosity of 4.9 fb-1, is used. The amount of
background, from hadronic jets and isolated electrons, is
estimated with data-driven techniques and subtracted. The
total cross section, for two isolated photons with
transverse energies above 25 GeV and 22 GeV respectively, in
the acceptance of the electromagnetic calorimeter (|η| <
1.37 and 1.52 < |η| < 2.37) and with an angular separation
ΔR > 0.4, is 44.0-4.2+3.2 pb. The differential cross
sections as a function of the di-photon invariant mass,
transverse momentum, azimuthal separation, and cosine of the
polar angle of the largest transverse energy photon in the
Collins-Soper di-photon rest frame are also measured. The
results are compared to the prediction of leading-order
parton-shower and next-to-leading-order and
next-to-next-to-leading-order parton-level
generators.[Figure not available: see fulltext.] © 2013
CERN for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP01(2013)086},
Key = {fds307645}
}
@article{fds349433,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP},
Title = {Measurement of isolated-photon plus two-jet production in pp
collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {3},
Year = {2020},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2020)179},
Abstract = {The dynamics of isolated-photon plus two-jet production in
pp collisions at a centre-of-mass energy of 13 TeV are
studied with the ATLAS detector at the LHC using a dataset
corresponding to an integrated luminosity of 36.1 fb−1.
Cross sections are measured as functions of a variety of
observables, including angular correlations and invariant
masses of the objects in the final state, γ + jet + jet.
Measurements are also performed in phase-space regions
enriched in each of the two underlying physical mechanisms,
namely direct and fragmentation processes. The measurements
cover the range of photon (jet) transverse momenta from 150
GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower
predictions from Sherpa and Pythia as well as the
next-to-leading-order QCD predictions from Sherpa are
compared with the measurements. The next-to-leading-order
QCD predictions describe the data adequately in shape and
normalisation except for regions of phase space such as
those with high values of the invariant mass or rapidity
separation of the two jets, where the predictions
overestimate the data. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP03(2020)179},
Key = {fds349433}
}
@article{fds356550,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Arduh, FA and Arguin,
JF},
Title = {Measurement of J/ψ production in association with a W
± boson with pp data at 8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {1},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2020)095},
Abstract = {A measurement of the production of a prompt J/ψ meson in
association with a W± boson with W± → μν and J/ψ →
μ+μ− is presented for J/ψ transverse momenta in the
range 8.5–150 GeV and rapidity |yJ/ψ| < 2.1 using ATLAS
data recorded in 2012 at the LHC. The data were taken at a
proton-proton centre-of-mass energy of s = 8 TeV and
correspond to an integrated luminosity of 20.3 fb−1. The
ratio of the prompt J/ψ plus W± cross-section to the
inclusive W± cross-section is presented as a differential
measurement as a function of J/ψ transverse momenta and
compared with theoretical predictions using different
double-parton-scattering cross-sections. [Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP01(2020)095},
Key = {fds356550}
}
@article{fds321095,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Measurement of jet activity in top quark events using the
eμ final state with two b-tagged jets in pp collisions at
√s=8 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)074},
Abstract = {Measurements of the jet activity in tt¯ events produced in
proton-proton collisions at s=8 TeV are presented, using
20.3 fb−1 of data collected by the ATLAS experiment at the
Large Hadron Collider. The events were selected in the
dilepton eμ decay channel with two identified b-jets. The
numbers of additional jets for various jet transverse
momentum (pT) thresholds, and the normalised differential
cross-sections as a function of pT for the five highest-pT
additional jets, were measured in the jet pseudo-rapidity
range |η| < 4.5. The gap fraction, the fraction of events
which do not contain an additional jet in a central rapidity
region, was measured for several rapidity intervals as a
function of the minimum pT of a single jet or the scalar sum
of pT of all additional jets. These fractions were also
measured in different intervals of the invariant mass of the
eμbb¯ system. All measurements were corrected for detector
effects, and found to be mostly well-described by
predictions from next-to-leading-order and leading-order
tt¯ event generators with appropriate parameter choices.
The results can be used to further optimise the parameters
used in such generators.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP09(2016)074},
Key = {fds321095}
}
@article{fds347497,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke,
S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda,
E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Measurement of jet activity produced in top-quark events
with an electron, a muon and two b-tagged jets in the
final state in pp collisions at [Formula: see text]
TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {4},
Pages = {220},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4766-0},
Abstract = {Measurements of jet activity in top-quark pair events
produced in proton-proton collisions are presented, using
3.2 fb[Formula: see text] of <i>pp</i> collision data at a
centre-of-mass energy of 13 TeV collected by the ATLAS
experiment at the Large Hadron Collider. Events are chosen
by requiring an opposite-charge [Formula: see text] pair and
two <i>b</i>-tagged jets in the final state. The normalised
differential cross-sections of top-quark pair production are
presented as functions of additional-jet multiplicity and
transverse momentum, [Formula: see text]. The fraction of
signal events that do not contain additional jet activity in
a given rapidity region, the gap fraction, is measured as a
function of the [Formula: see text] threshold for additional
jets, and is also presented for different invariant mass
regions of the [Formula: see text] system. All measurements
are corrected for detector effects and presented as
particle-level distributions compared to predictions with
different theoretical approaches for QCD radiation. While
the kinematics of the jets from top-quark decays are
described well, the generators show differing levels of
agreement with the measurements of observables that depend
on the production of additional jets.},
Doi = {10.1140/epjc/s10052-017-4766-0},
Key = {fds347497}
}
@article{fds356779,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Measurement of jet charge in dijet events from s =8 TeV pp
collisions with the ATLAS detector},
Journal = {Physical Review D},
Volume = {93},
Number = {5},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.93.052003},
Abstract = {The momentum-weighted sum of the charges of tracks
associated to a jet is sensitive to the charge of the
initiating quark or gluon. This paper presents a measurement
of the distribution of momentum-weighted sums, called jet
charge, in dijet events using 20.3 fb-1 of data recorded
with the ATLAS detector at s=8 TeV in pp collisions at the
LHC. The jet charge distribution is unfolded to remove
distortions from detector effects and the resulting
particle-level distribution is compared with several models.
The pT dependence of the jet charge distribution average and
standard deviation are compared to predictions obtained with
several leading-order and next-to-leading-order parton
distribution functions. The data are also compared to
different Monte Carlo simulations of QCD dijet production
using various settings of the free parameters within these
models. The chosen value of the strong coupling constant
used to calculate gluon radiation is found to have a
significant impact on the predicted jet charge. There is
evidence for a pT dependence of the jet charge distribution
for a given jet flavor. In agreement with perturbative QCD
predictions, the data show that the average jet charge of
quark-initiated jets decreases in magnitude as the energy of
the jet increases.},
Doi = {10.1103/PhysRevD.93.052003},
Key = {fds356779}
}
@article{fds356653,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
H},
Title = {Measurement of jet fragmentation in 5.02 TeV proton–lead
and proton–proton collisions with the ATLAS
detector},
Journal = {Nuclear Physics A},
Volume = {978},
Pages = {65-106},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1016/j.nuclphysa.2018.07.006},
Abstract = {A measurement of the fragmentation functions of jets into
charged particles in p+Pb collisions and pp collisions is
presented. The analysis utilizes 28 nb−1 of p+Pb data and
26 pb−1 of pp data, both at sNN= 5.02 TeV, collected in
2013 and 2015, respectively, with the ATLAS detector at the
LHC. The measurement is reported in the centre-of-mass frame
of the nucleon–nucleon system for jets in the rapidity
range |y⁎|<1.6 and with transverse momentum 45 <pT< 260
GeV. Results are presented both as a function of the
charged-particle transverse momentum and as a function of
the longitudinal momentum fraction of the particle with
respect to the jet. The pp fragmentation functions are
compared with results from Monte Carlo event generators and
two theoretical models. The ratios of the p+Pb to pp
fragmentation functions are found to be consistent with
unity.},
Doi = {10.1016/j.nuclphysa.2018.07.006},
Key = {fds356653}
}
@article{fds347502,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin,
DL and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke,
S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini,
I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
Title = {Measurement of jet fragmentation in Pb+Pb and pp
collisions at sNN=2.76 TeV with the ATLAS detector at the
LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {6},
Pages = {379},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4915-5},
Abstract = {The distributions of transverse momentum and longitudinal
momentum fraction of charged particles in jets are measured
in Pb+Pb and <i>pp</i> collisions with the ATLAS detector at
the LHC. The distributions are measured as a function of jet
transverse momentum and rapidity. The analysis utilises an
integrated luminosity of 0.14 nb -1 of Pb+Pb data and 4.0 pb
-1 of <i>pp</i> data collected in 2011 and 2013,
respectively, at the same centre-of-mass energy of 2.76 TeV
per colliding nucleon pair. The distributions measured in
<i>pp</i> collisions are used as a reference for those
measured in Pb+Pb collisions in order to evaluate the impact
on the internal structure of jets from the jet energy loss
of fast partons propagating through the hot, dense medium
created in heavy-ion collisions. Modest but significant
centrality-dependent modifications of fragmentation
functions in Pb+Pb collisions with respect to those in
<i>pp</i> collisions are seen. No significant dependence of
modifications on jet pT and rapidity selections is observed
except for the fragments with the highest transverse momenta
for which some reduction of yields is observed for more
forward jets.},
Doi = {10.1140/epjc/s10052-017-4915-5},
Key = {fds347502}
}
@article{fds356666,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H},
Title = {Measurement of jet fragmentation in Pb+Pb and pp collisions
at sNN =5.02 TeV with the ATLAS detector},
Journal = {Physical Review C},
Volume = {98},
Number = {2},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevC.98.024908},
Abstract = {This paper presents a measurement of jet fragmentation
functions in 0.49 nb-1 of Pb+Pb collisions and 25 pb-1 of pp
collisions at sNN=5.02 TeV collected in 2015 with the ATLAS
detector at the LHC. These measurements provide insight into
the jet quenching process in the quark-gluon plasma created
in the aftermath of ultrarelativistic collisions between two
nuclei. The modifications to the jet fragmentation functions
are quantified by dividing the measurements in Pb+Pb
collisions by baseline measurements in pp collisions. This
ratio is studied as a function of the transverse momentum of
the jet, the jet rapidity, and the centrality of the
collision. In both collision systems, the jet fragmentation
functions are measured for jets with transverse momentum
between 126 and 398 GeV and with an absolute value of jet
rapidity less than 2.1. An enhancement of particles carrying
a small fraction of the jet momentum is observed, which
increases with centrality and with increasing jet transverse
momentum. Yields of particles carrying a very large fraction
of the jet momentum are also observed to be enhanced.
Between these two enhancements of the fragmentation
functions a suppression of particles carrying an
intermediate fraction of the jet momentum is observed in
Pb+Pb collisions. A small dependence of the modifications on
jet rapidity is observed.},
Doi = {10.1103/PhysRevC.98.024908},
Key = {fds356666}
}
@article{fds356724,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of jet pT correlations in Pb + Pb and
pp collisions at sNN=2.76 TeVwith the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {774},
Pages = {379-402},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2017.09.078},
Abstract = {Measurements of dijet pT correlations in Pb+Pb and pp
collisions at a nucleon–nucleon centre-of-mass energy of
sNN=2.76 TeV are presented. The measurements are performed
with the ATLAS detector at the Large Hadron Collider using
Pb+Pb and pp data samples corresponding to integrated
luminosities of 0.14 nb−1 and 4.0 pb−1, respectively.
Jets are reconstructed using the anti-kt algorithm with
radius parameter values R=0.3 and R=0.4. A background
subtraction procedure is applied to correct the jets for the
large underlying event present in Pb+Pb collisions. The
leading and sub-leading jet transverse momenta are denoted
pT1 and pT2. An unfolding procedure is applied to the
two-dimensional (pT1,pT2) distributions to account for
experimental effects in the measurement of both jets.
Distributions of (1/N)dN/dxJ, where xJ=pT2/pT1, are
presented as a function of pT1 and collision centrality. The
distributions are found to be similar in peripheral Pb+Pb
collisions and pp collisions, but highly modified in central
Pb+Pb collisions. Similar features are present in both the
R=0.3 and R=0.4 results, indicating that the effects of the
underlying event are properly accounted for in the
measurement. The results are qualitatively consistent with
expectations from partonic energy loss models.},
Doi = {10.1016/j.physletb.2017.09.078},
Key = {fds356724}
}
@article{fds307642,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat,
P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiarella,
V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
RN},
Title = {Measurement of jet shapes in top-quark pair events at
[Formula: see text] using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {12},
Pages = {2676},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2676-3},
Abstract = {A measurement of jet shapes in top-quark pair events using
1.8 fb<sup>-1</sup> of [Formula: see text]<i>pp</i>
collision data recorded by the ATLAS detector at the LHC is
presented. Samples of top-quark pair events are selected in
both the single-lepton and dilepton final states. The
differential and integrated shapes of the jets initiated by
bottom-quarks from the top-quark decays are compared with
those of the jets originated by light-quarks from the
hadronic <i>W</i>-boson decays [Formula: see text] in the
single-lepton channel. The light-quark jets are found to
have a narrower distribution of the momentum flow inside the
jet area than <i>b</i>-quark jets.},
Doi = {10.1140/epjc/s10052-013-2676-3},
Key = {fds307642}
}
@article{fds356584,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP},
Title = {Measurement of jet-substructure observables in top quark, W
boson and light jet production in proton-proton collisions
at √s = 13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {8},
Year = {2019},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2019)033},
Abstract = {A measurement of jet substructure observables is presented
using data collected in 2016 by the ATLAS experiment at the
LHC with proton-proton collisions at s = 13 TeV.
Large-radius jets groomed with the trimming and soft-drop
algorithms are studied. Dedicated event selections are used
to study jets produced by light quarks or gluons, and
hadronically decaying top quarks and W bosons. The
observables measured are sensitive to substructure, and
therefore are typically used for tagging large-radius jets
from boosted massive particles. These include the energy
correlation functions and the N-subjettiness variables. The
number of subjets and the Les Houches angularity are also
considered. The distributions of the substructure variables,
corrected for detector effects, are compared to the
predictions of various Monte Carlo event generators. They
are also compared between the large-radius jets originating
from light quarks or gluons, and hadronically decaying top
quarks and W bosons. [Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP08(2019)033},
Key = {fds356584}
}
@article{fds356556,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
Title = {Measurement of KS0 and Λ production in tt¯ dileptonic
events in pp collisions at √s= 7 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {12},
Year = {2019},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7512-y},
Abstract = {Measurements of KS0 and Λ production in tt¯ final states
have been performed. They are based on a data sample with
integrated luminosity of 4.6 fb - 1 from proton–proton
collisions at a centre-of-mass energy of 7 TeV, collected in
2011 with the ATLAS detector at the Large Hadron Collider.
Neutral strange particles are separated into three classes,
depending on whether they are contained in a jet, with or
without a b-tag, or not associated with a selected jet. The
aim is to look for differences in their main kinematic
distributions. A comparison of data with several Monte Carlo
simulations using different hadronisation and fragmentation
schemes, colour reconnection models and different tunes for
the underlying event has been made. The production of
neutral strange particles in tt¯ dileptonic events is found
to be well described by current Monte Carlo models for KS0
and Λ production within jets, but not for those produced
outside jets.},
Doi = {10.1140/epjc/s10052-019-7512-y},
Key = {fds356556}
}
@article{fds348985,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
Title = {Measurement of lepton differential distributions and the top
quark mass in t t ¯ production in pp collisions at s
= 8 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {11},
Pages = {804},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5349-9},
Abstract = {This paper presents single lepton and dilepton kinematic
distributions measured in dileptonic t t ¯ events produced
in 20.2 fb - 1 of s = 8 TeV <i>pp</i> collisions recorded
by the ATLAS experiment at the LHC. Both absolute and
normalised differential cross-sections are measured, using
events with an opposite-charge e μ pair and one or two
<i>b</i>-tagged jets. The cross-sections are measured in a
fiducial region corresponding to the detector acceptance for
leptons, and are compared to the predictions from a variety
of Monte Carlo event generators, as well as fixed-order QCD
calculations, exploring the sensitivity of the
cross-sections to the gluon parton distribution function.
Some of the distributions are also sensitive to the top
quark pole mass; a combined fit of NLO fixed-order
predictions to all the measured distributions yields a top
quark mass value of m t pole = 173.2 ± 0.9 ± 0.8 ± 1.2
GeV, where the three uncertainties arise from data
statistics, experimental systematics, and theoretical
sources.},
Doi = {10.1140/epjc/s10052-017-5349-9},
Key = {fds348985}
}
@article{fds355784,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Measurement of light-by-light scattering and search for
axion-like particles with 2.2 nb−1 of Pb+Pb
data with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {3},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2021)243},
Abstract = {This paper describes a measurement of light-by-light
scattering based on Pb+Pb collision data recorded by the
ATLAS experiment during Run 2 of the LHC. The study uses 2.2
nb−1 of integrated luminosity collected in 2015 and 2018
at sNN = 5.02 TeV. Light-by-light scattering candidates are
selected in events with two photons produced exclusively,
each with transverse energy ETγ> 2.5 GeV, pseudorapidity
|ηγ| < 2.37, diphoton invariant mass mγγ> 5 GeV, and
with small diphoton transverse momentum and diphoton
acoplanarity. The integrated and differential fiducial cross
sections are measured and compared with theoretical
predictions. The diphoton invariant mass distribution is
used to set limits on the production of axion-like
particles. This result provides the most stringent limits to
date on axion-like particle production for masses in the
range 6–100 GeV. Cross sections above 2 to 70 nb are
excluded at the 95% CL in that mass interval. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP03(2021)243},
Key = {fds355784}
}
@article{fds356696,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of long-range multiparticle azimuthal
correlations with the subevent cumulant method in pp and p
+Pb collisions with the ATLAS detector at the CERN Large
Hadron Collider},
Journal = {Physical Review C},
Volume = {97},
Number = {2},
Year = {2018},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevC.97.024904},
Abstract = {A detailed study of multiparticle azimuthal correlations is
presented using pp data at s=5.02 and 13 TeV, and p+Pb data
at sNN=5.02 TeV, recorded with the ATLAS detector at the
CERN Large Hadron Collider. The azimuthal correlations are
probed using four-particle cumulants cn{4} and flow
coefficients vn{4}=(-cn{4})1/4 for n=2 and 3, with the goal
of extracting long-range multiparticle azimuthal correlation
signals and suppressing the short-range correlations. The
values of cn{4} are obtained as a function of the average
number of charged particles per event, Nch, using the
recently proposed two-subevent and three-subevent cumulant
methods, and compared with results obtained with the
standard cumulant method. The standard method is found to be
strongly biased by short-range correlations, which originate
mostly from jets with a positive contribution to cn{4}. The
three-subevent method, on the other hand, is found to be
least sensitive to short-range correlations. The
three-subevent method gives a negative c2{4}, and therefore
a well-defined v2{4}, nearly independent of Nch, which
implies that the long-range multiparticle azimuthal
correlations persist to events with low multiplicity.
Furthermore, v2{4} is found to be smaller than the v2{2}
measured using the two-particle correlation method, as
expected for long-range collective behavior. Finally, the
measured values of v2{4} and v2{2} are used to estimate the
number of sources relevant for the initial eccentricity in
the collision geometry. The results based on the subevent
cumulant technique provide direct evidence, in small
collision systems, for a long-range collectivity involving
many particles distributed across a broad rapidity
interval.},
Doi = {10.1103/PhysRevC.97.024904},
Key = {fds356696}
}
@article{fds310353,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of long-range pseudorapidity correlations and
azimuthal harmonics in √sNN =5.02 TeV
proton-lead collisions with the ATLAS detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {90},
Number = {4},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevC.90.044906},
Abstract = {Measurements of two-particle correlation functions and the
first five azimuthal harmonics, v1 to v5, are presented,
using 28 nb-1 of p+Pb collisions at a nucleon-nucleon
center-of-mass energy of √sNN=5.02 TeV measured with the
ATLAS detector at the LHC. Significant long-range
"ridgelike" correlations are observed for pairs with small
(|Δϕ|<π/3) and back-to-back pairs (|Δφ|>2π/3) over the
transverse momentum range 0.4<pT<12 GeV and in different
intervals of event activity. The event activity is defined
by either the number of reconstructed tracks or the total
transverse energy on the Pb-fragmentation side. The
azimuthal structure of such long-range correlations is
Fourier decomposed to obtain the harmonics νn as a function
of pT and event activity. The extracted νn values for n=2
to 5 decrease with n. The ν2 and ν3 values are found to be
positive in the measured pT range. The ν1 is also measured
as a function of pT and is observed to change sign around
pT≈1.5-2.0 GeV and then increase to about 0.1 for pT>4
GeV. The ν2 (pT), ν3 (pT), and ν4 (pT) are compared to
the νn coefficients in Pb+Pb collisions at √sNN=2.76 TeV
with similar event multiplicities. Reasonable agreement is
observed after accounting for the difference in the average
pT of particles produced in the two collision
systems.},
Doi = {10.1103/PhysRevC.90.044906},
Key = {fds310353}
}
@article{fds356549,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arling,
JH},
Title = {Measurement of long-range two-particle azimuthal
correlations in Z-boson tagged pp collisions at √s=8 and
13 TeV},
Journal = {European Physical Journal C},
Volume = {80},
Number = {1},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-7606-6},
Abstract = {Results are presented from the measurement by ATLAS of
long-range (| Δ η| > 2) dihadron angular correlations in
s=8 and 13 TeV pp collisions containing a Z boson. The
analysis is performed using 19.4 fb - 1 of s=8 TeV data
recorded during Run 1 of the LHC and 36.1 fb - 1 of
s=13 TeV data recorded during Run 2. Two-particle
correlation functions are measured as a function of relative
azimuthal angle over the relative pseudorapidity range 2 < |
Δ η| < 5 for different intervals of charged-particle
multiplicity and transverse momentum. The measurements are
corrected for the presence of background charged particles
generated by collisions that occur during one passage of two
colliding proton bunches in the LHC. Contributions to the
two-particle correlation functions from hard processes are
removed using a template-fitting procedure. Sinusoidal
modulation in the correlation functions is observed and
quantified by the second Fourier coefficient of the
correlation function, v2 , 2, which in turn is used to
obtain the single-particle anisotropy coefficient v2. The v2
values in the Z-tagged events, integrated over 0.5 < pT< 5
GeV, are found to be independent of multiplicity and s, and
consistent within uncertainties with previous measurements
in inclusive pp collisions. As a function of
charged-particle pT, the Z-tagged and inclusive v2 values
are consistent within uncertainties for pT< 3
GeV.},
Doi = {10.1140/epjc/s10052-020-7606-6},
Key = {fds356549}
}
@article{fds347469,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
Title = {Measurement of longitudinal flow decorrelations in Pb+Pb
collisions at s NN = 2.76 and 5.02 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {2},
Pages = {142},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5605-7},
Abstract = {Measurements of longitudinal flow correlations are presented
for charged particles in the pseudorapidity range | η | <
2.4 using 7 and 470 μ b - 1 of Pb+Pb collisions at s NN =
2.76 and 5.02 TeV, respectively, recorded by the ATLAS
detector at the LHC. It is found that the correlation
between the harmonic flow coefficients v n measured in two
separated η intervals does not factorise into the product
of single-particle coefficients, and this breaking of
factorisation, or flow decorrelation, increases linearly
with the η separation between the intervals. The flow
decorrelation is stronger at 2.76 TeV than at 5.02 TeV.
Higher-order moments of the correlations are also measured,
and the corresponding linear coefficients for the k th
-moment of the v n are found to be proportional to <i>k</i>
for v 3 , but not for v 2 . The decorrelation effect is
separated into contributions from the magnitude of v n and
the event-plane orientation, each as a function of η .
These two contributions are found to be comparable. The
longitudinal flow correlations are also measured between v n
of different order in <i>n</i>. The decorrelations of v 2
and v 3 are found to be independent of each other, while the
decorrelations of v 4 and v 5 are found to be driven by the
nonlinear contribution from v 2 2 and v 2 v 3 ,
respectively.},
Doi = {10.1140/epjc/s10052-018-5605-7},
Key = {fds347469}
}
@article{fds308109,
Author = {Abulencia, and A, and others},
Title = {Measurement of mass and width of the excited charmed meson
states D10 and D2*0},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {5},
Pages = {051104},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.051104},
Abstract = {We report on precision measurements of the masses and widths
of the narrow, orbitally excited states D0_1 and D*0_2 using
the CDF II detector at the Fermilab Tevatron. Both states
(collectively called D**) are reconstructed in the decay
channel D** --> D*+ pi+-. The D*0_s is also reconstructed in
the D** --> D+ pi+- channel. Using a dataset with an
integrated luminosity of 210 pb-1, the measured masses and
widths for the D0_1 are 2421.7 +/- 0.7 +/- 0.6 MeV/c2 and
20.0 +/- 1.7 +/- 1.3 MeV/c2 respectively, while for the
D*0_2 they are 2463.3 +/- 0.6 +/- 0.8 MeV/c2 and 49.2 +/-
2.3 +/- 1.2 MeV/c2. These values are currently the single
best measurements available.},
Doi = {10.1103/PhysRevD.73.051104},
Key = {fds308109}
}
@article{fds325779,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Measurement of multi-jet cross sections in proton–proton
collisions at a 7 TeV center-of-mass energy},
Journal = {European Physical Journal C},
Volume = {71},
Number = {11},
Pages = {1-27},
Publisher = {Springer Nature},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1763-6},
Abstract = {Inclusive multi-jet production is studied in proton–proton
collisions at a center-of-mass energy of 7 TeV, using the
ATLAS detector. The data sample corresponds to an integrated
luminosity of 2.4 pb-1. Results on multi-jet cross sections
are presented and compared to both leading-order plus
parton-shower Monte Carlo predictions and to
next-to-leading-order QCD calculations.},
Doi = {10.1140/epjc/s10052-011-1763-6},
Key = {fds325779}
}
@article{fds347506,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa,
M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos,
SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic,
M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul,
A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard,
DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair,
RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin,
DL and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burch, TJ and Burckhart, H and Burdin,
S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke,
S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán,
SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura,
P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone,
RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino,
G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn,
R and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca,
D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A},
Title = {Measurement of multi-particle azimuthal correlations in pp,
p + Pb and low-multiplicity Pb + Pb collisions with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {6},
Pages = {428},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4988-1},
Abstract = {Multi-particle cumulants and corresponding Fourier harmonics
are measured for azimuthal angle distributions of charged
particles in [Formula: see text] collisions at [Formula: see
text] = 5.02 and 13 TeV and in [Formula: see text] + Pb
collisions at [Formula: see text] = 5.02 TeV, and compared
to the results obtained for low-multiplicity [Formula: see
text] collisions at [Formula: see text] = 2.76 TeV. These
measurements aim to assess the collective nature of particle
production. The measurements of multi-particle cumulants
confirm the evidence for collective phenomena in [Formula:
see text] + Pb and low-multiplicity [Formula: see text]
collisions. On the other hand, the [Formula: see text]
results for four-particle cumulants do not demonstrate
collective behaviour, indicating that they may be biased by
contributions from non-flow correlations. A comparison of
multi-particle cumulants and derived Fourier harmonics
across different collision systems is presented as a
function of the charged-particle multiplicity. For a given
multiplicity, the measured Fourier harmonics are largest in
[Formula: see text], smaller in [Formula: see text] + Pb
and smallest in [Formula: see text] collisions. The
[Formula: see text] results show no dependence on the
collision energy, nor on the multiplicity.},
Doi = {10.1140/epjc/s10052-017-4988-1},
Key = {fds347506}
}
@article{fds372394,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Measurement of muon pairs produced via γγ scattering in
nonultraperipheral Pb + Pb collisions at √sNN = 5.02 TeV
with the ATLAS detector},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054907},
Abstract = {Results of a measurement of dimuon photoproduction in
nonultraperipheral Pb + Pb collisions at √sNN = 5.02 TeV
are presented. Themeasurement uses ATLAS data from the 2015
and 2018 Pb + Pb data-taking periods at the LHC with an
integrated luminosity of 1.94 nb.1. The γγ → μ+ μ-
pairs are identified via selections on pair momentum
asymmetry and acoplanarity. Differential cross sections for
dimuon production are measured in different centrality,
average muon momentum, and pair rapidity intervals as
functions of acoplanarity and k⊥, the transverse momentum
kick of one muon relative to the other. Measurements are
also made as a function of the rapidity separation of the
muons and the angle of the muon pair relative to the
second-order event plane to test whether magnetic fields
generated in the quark-gluon plasma affect the measured
muons. A prior observation of a centrality-dependent
broadening of the acoplanarity distribution is confirmed.
Furthermore, the improved precision of the measurement
reveals a depletion in the number of pairs having small
acoplanarity or k⊥ values in more central collisions. The
acoplanarity distributions in a given centrality interval
are observed to vary with the mean pT of the muons in the
pair, but the k⊥ distributions do not. Comparisons with
recent theoretical predictions are made. The predicted
trends associated with effects of magnetic fields on the
dimuons are not observed.},
Doi = {10.1103/PhysRevC.107.054907},
Key = {fds372394}
}
@booklet{Adams95c,
Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Breidung, H and Busza, W and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dhawan, SK and Dietrich, FS and Dougherty,
W and Dreyer, T and Eckardt, V and Ecker, U and Erdmann, M and Faller, F and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Hughes, VW and Jackson, HE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kirk, T and Kobrak, HG and Kotwal, AV and Kunori, S and Lancaster, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and O'Day, S and Olkiewicz, K and Osborne, L and Otten,
R},
Title = {Measurement of nuclear transparencies from exclusive rho 0
meson production in muon-nucleus scattering at 470
GeV.},
Journal = {Physical review letters},
Volume = {74},
Number = {9},
Pages = {1525-1529},
Year = {1995},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.74.1525},
Doi = {10.1103/physrevlett.74.1525},
Key = {Adams95c}
}
@article{fds308156,
Author = {Acosta, D and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli, M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, J and Frisch,
H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic,
P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin,
A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa,
T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patricck, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio,
S and Ratnikov, F and Ray, H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna,
G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar,
S and Sato, K and Savard, P and Savoy-Navarro, A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet,
M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smirnov, D and Smith, JR and Snider,
FD},
Title = {Measurement of partial widths and search for direct CP
violation in D 0 meson decays to
K-K+ and π -π+},
Journal = {Physical Review Letters},
Volume = {94},
Number = {12},
Pages = {122001},
Year = {2005},
ISSN = {0031-9007},
url = {http://www.ncbi.nlm.nih.gov/pubmed/15903906},
Abstract = {We present a measurement of relative partial widths and
decay rate CP asymmetries in K- K+ and π-π+ decays of D0
mesons produced in pp̄ collisions at,√s = 1.96 TeV. We
use a sample of 2 × 105 D*+ →D0π+ (and charge conjugate)
decays with the D0 decaying to K-π+, K-K +, and π-π+,
corresponding to 123 pb -1 of data collected by the Collider
Detector at Fermilab II experiment at the Fermilab Tevatron
collider. No significant direct CP violation is observed. We
measure γ(D0→ K- K +)/γ(D0-→K-π+) = 0.0992 ±0.0992
±0.0012, γ(D0→K -π+)/γ(D0→K -π+) = 0.03594 ±
0.00054 ±0.00040, A CP(K- K+) = (2.0 ±1.2 ±0.6)%, and
ACP(π-π+) = (1.0 ±1.3 ±0.6)%, where, in all cases, the
first uncertainty is statistical and the second is
systematic. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.94.122001},
Key = {fds308156}
}
@article{fds307993,
Author = {Aaltonen, T and others},
Title = {Measurement of particle production and inclusive
differential cross sections in pp̅ collisions at sqrt[s]
=1.96 TeV},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {11},
Pages = {112005},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112005},
Abstract = {We report a set of measurements of particle production in
inelastic pp̅ collisions collected with a minimum-bias
trigger at the Tevatron Collider with the CDF II experiment.
The inclusive charged particle transverse momentum
differential cross section is measured, with improved
precision, over a range about ten times wider than in
previous measurements. The former modeling of the spectrum
appears to be incompatible with the high particle momenta
observed. The dependence of the charged particle transverse
momentum on the event particle multiplicity is analyzed to
study the various components of hadron interactions. This is
one of the observable variables most poorly reproduced by
the available Monte Carlo generators. A first measurement of
the event transverse energy sum differential cross section
is also reported. A comparison with a pythia prediction at
the hadron level is performed. The inclusive
charged-particle differential production cross section is
fairly well reproduced only in the transverse momentum range
available from previous measurements. At higher momentum the
agreement is poor. The transverse energy sum is poorly
reproduced over the whole spectrum. The dependence of the
charged particle transverse momentum on the particle
multiplicity needs the introduction of more sophisticated
particle production mechanisms, such as multiple parton
interactions, in order to be better explained.},
Doi = {10.1103/PhysRevD.79.112005},
Key = {fds307993}
}
@article{fds356624,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Measurement of photon–jet transverse momentum correlations
in 5.02 TeV Pb + Pb and pp collisions with
ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {789},
Pages = {167-190},
Year = {2019},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2018.12.023},
Abstract = {Jets created in association with a photon can be used as a
calibrated probe to study energy loss in the medium created
in nuclear collisions. Measurements of the transverse
momentum balance between isolated photons and inclusive jets
are presented using integrated luminosities of 0.49 nb−1
of Pb + Pb collision data at sNN=5.02 TeV and 25 pb−1 of
pp collision data at s=5.02 TeV recorded with the ATLAS
detector at the LHC. Photons with transverse momentum
63.1<pTγ<200 GeV and |ηγ|<2.37 are paired with all jets
in the event that have pTjet>31.6 GeV and pseudorapidity
|ηjet|<2.8. The transverse momentum balance given by the
jet-to-photon pT ratio, xJγ, is measured for pairs with
azimuthal opening angle Δϕ>7π/8. Distributions of the
per-photon jet yield as a function of xJγ,
(1/Nγ)(dN/dxJγ), are corrected for detector effects via a
two-dimensional unfolding procedure and reported at the
particle level. In pp collisions, the distributions are well
described by Monte Carlo event generators. In Pb + Pb
collisions, the xJγ distribution is modified from that
observed in pp collisions with increasing centrality,
consistent with the picture of parton energy loss in the hot
nuclear medium. The data are compared with a suite of
energy-loss models and calculations.},
Doi = {10.1016/j.physletb.2018.12.023},
Key = {fds356624}
}
@article{fds307829,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rosner, JL and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester,
WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang,
YC},
Title = {Measurement of polarization and search for CP violation in
B(s)0→φφ decays.},
Journal = {Physical review letters},
Volume = {107},
Number = {26},
Pages = {261802},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.107.261802},
Abstract = {We present the first measurement of polarization and
CP-violating asymmetries in a B(s)(0) decay into two light
vector mesons, B(s)(0)→φφ, and an improved determination
of its branching ratio using 295 decays reconstructed in a
data sample corresponding to 2.9 fb(-1) of integrated
luminosity collected by the CDF experiment at the Fermilab
Tevatron collider. The fraction of longitudinal polarization
is determined to be f(L)=0.348±0.041(stat)±0.021(syst),
and the branching ratio B(B(s)(0)→φφ)=[2.32±0.18(stat)±0.82(syst)]×10(-5).
Asymmetries of decay angle distributions sensitive to CP
violation are measured to be A(u)=-0.007±0.064(stat)±0.018(syst)
and A(v)=-0.120±0.064(stat)±0.016(syst).},
Doi = {10.1103/physrevlett.107.261802},
Key = {fds307829}
}
@article{fds308167,
Author = {Collaboration, DAEACDFII},
Title = {Measurement of Prompt Charm Meson Production Cross Sections
in pp-bar Collisions at sqrt[s]=1.96 TeV},
Journal = {Physical Review Letters},
Volume = {91},
Number = {24},
Pages = {241804},
Year = {2003},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.91.241804},
Abstract = {We report on measurements of differential cross sections d
sigma /dpT for prompt charm meson production in pp-bar
collisions at sqrt[s]=1.96 TeV using 5.8±0.3 pb-1 of data
from the CDF II detector at the Fermilab Tevatron. The data
are collected with a new trigger that is sensitive to the
long lifetime of hadrons containing heavy flavor. The charm
meson cross sections are measured in the central rapidity
region |y| K- pi +, D*+-->D0 pi +, D+-->K- pi + pi +, D+s-->
phi pi +, and their charge conjugates. The measured cross
sections are compared to theoretical calculations.},
Doi = {10.1103/physrevlett.91.241804},
Key = {fds308167}
}
@article{fds356576,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
JF},
Title = {Measurement of prompt photon production in
sNN=8.16 TeV p + Pb collisions with
ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {796},
Pages = {230-252},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2019.07.031},
Abstract = {The inclusive production rates of isolated, prompt photons
in p+Pb collisions at sNN=8.16 TeV are studied with the
ATLAS detector at the Large Hadron Collider using a dataset
with an integrated luminosity of 165 nb−1 recorded in
2016. The cross-section and nuclear modification factor RpPb
are measured as a function of photon transverse energy from
20 GeV to 550 GeV and in three nucleon–nucleon
centre-of-mass pseudorapidity regions, (−2.83,−2.02),
(−1.84,0.91), and (1.09,1.90). The cross-section and RpPb
values are compared with the results of a
next-to-leading-order perturbative QCD calculation, with and
without nuclear parton distribution function modifications,
and with expectations based on a model of the energy loss of
partons prior to the hard scattering. The data disfavour a
large amount of energy loss and provide new constraints on
the parton densities in nuclei.},
Doi = {10.1016/j.physletb.2019.07.031},
Key = {fds356576}
}
@article{fds347470,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A},
Title = {Measurement of quarkonium production in proton-lead and
proton-proton collisions at 5.02 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {3},
Pages = {171},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5624-4},
Abstract = {The modification of the production of J / ψ , ψ ( 2 S ) ,
and Υ ( n S ) ( n = 1 , 2 , 3 ) in <i>p</i>+Pb collisions
with respect to their production in <i>pp</i> collisions has
been studied. The <i>p</i>+Pb and <i>pp</i> datasets used in
this paper correspond to integrated luminosities of 28 nb -
1 and 25 pb - 1 respectively, collected in 2013 and 2015 by
the ATLAS detector at the LHC, both at a centre-of-mass
energy per nucleon pair of 5.02 TeV. The quarkonium states
are reconstructed in the dimuon decay channel. The yields of
J / ψ and ψ ( 2 S ) are separated into prompt and
non-prompt sources. The measured quarkonium differential
cross sections are presented as a function of rapidity and
transverse momentum, as is the nuclear modification factor,
R p Pb for J / ψ and Υ ( n S ) . No significant
modification of the J / ψ production is observed while Υ (
n S ) production is found to be suppressed at low transverse
momentum in <i>p</i>+Pb collisions relative to <i>pp</i>
collisions. The production of excited charmonium and
bottomonium states is found to be suppressed relative to
that of the ground states in central <i>p</i>+Pb
collisions.},
Doi = {10.1140/epjc/s10052-018-5624-4},
Key = {fds347470}
}
@article{fds307599,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Measurement of R=B(t→Wb)/B(t→Wq) in top-quark-pair
decays using lepton+jets events and the full CDF run II
dataset},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.87.111101},
Abstract = {We present a measurement of the ratio of the top-quark
branching fractions R=B(t→Wb)/B(t→Wq), where q
represents quarks of type b, s, or d, in the final state
with a lepton and hadronic jets. The measurement uses
√s=1.96 TeV proton-antiproton collision data from 8.7 fb-1
of integrated luminosity collected with the Collider
Detector at Fermilab during Run II of the Tevatron. We
simultaneously measure R=0.94±0.09 (stat+syst) and the tt̄
production cross section σtt̄=7. 5±1.0 (stat+syst) pb.
The magnitude of the Cabibbo-Kobayashi-Maskawa matrix
element, |Vtb|=0.97±0.05 (stat+syst) is extracted assuming
three generations of quarks, and a lower limit of |V
tb|>0.89 at 95% credibility level is set. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.87.111101},
Key = {fds307599}
}
@article{fds307957,
Author = {Aaltonen, T and others},
Title = {Measurement of Resonance Parameters of Orbitally Excited
Narrow B[sup 0] Mesons},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {10},
Pages = {102003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.102003},
Abstract = {We report a measurement of resonance parameters of the
orbitally excited (L=1) narrow B0 mesons in decays to
B;{(*)+}pi;{-} using 1.7 fb;{-1} of data collected by the
CDF II detector at the Fermilab Tevatron. The mass and width
of the B_{2};{*0} state are measured to be
m(B_{2};{*0})=5740.2_{-1.8};{+1.7}(stat)-0.8+0.9(syst)
MeV/c;{2} and Gamma(B_{2};{*0})=22.7_{-3.2};{+3.8}(stat)-10.2+3.2(syst)
MeV/c;{2}. The mass difference between the B_{2};{*0} and
B10 states is measured to be 14.9_{-2.5};{+2.2}(stat)-1.4+1.2(syst)
MeV/c;{2}, resulting in a B10 mass of 5725.3_{-2.2};{+1.6}(stat)-1.5+1.4(syst)
MeV/c;{2}. This is currently the most precise measurement of
the masses of these states and the first measurement of the
B_{2};{*0} width.},
Doi = {10.1103/physrevlett.102.102003},
Key = {fds307957}
}
@article{fds308080,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Cyr,
D and DaRonco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De
Lentdecker, G and Dell'Orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni,
GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and DiTuro, P and Dörr,
C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell,
JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Guimaraes da
Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Le, Y and LeCompte, T and Lee, J and Lee,
YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean,
R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Movilla
Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ranjan,
N and Rappoccio, S and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin, J},
Title = {Measurement of sigma Lambda b0/sigma B0 x B(Lambda
b0-->Lambda c+pi-)/B(B0-->D+pi-) in pp collisions at square
root s=1.96 TeV.},
Journal = {Physical review letters},
Volume = {98},
Number = {12},
Pages = {122002},
Year = {2007},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.98.122002},
Abstract = {We present the first observation of the baryon decay Lambda
b0-->Lambda c+pi- followed by Lambda c+-->pK-pi+ in 106 pb-1
pp collisions at square root s=1.96 TeV in the CDF
experiment. In order to reduce systematic error, the
measured rate for Lambda b0 decay is normalized to the
kinematically similar meson decay B0-->D+pi- followed by
D+-->pi+K-pi+. We report the ratio of production cross
sections (sigma) times the ratio of branching fractions (B)
for the momentum region integrated above pT>6 GeV/c and
pseudorapidity range |eta|<1.3: sigma(pp-->Lambda
b0X)/sigma(pp-->B0X)xB(Lambda b0-->Lambda
c+pi-)/B(B0-->D+pi-)=0.82+/-0.08(stat)+/-0.11(syst)+/-0.22[B(Lambda
c+-->pK-pi+)].},
Doi = {10.1103/physrevlett.98.122002},
Key = {fds308080}
}
@article{fds321122,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Measurement of sin2 θefflept
using e+e- pairs from γ∗/Z bosons produced in
pp collisions at a center-of-momentum energy of 1.96
TeV},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112016},
Abstract = {At the Fermilab Tevatron proton-antiproton (pp) collider,
Drell-Yan lepton pairs are produced in the process
pp→e+e-+X through an intermediate γ∗/Z boson. The
forward-backward asymmetry in the polar-angle distribution
of the e- as a function of the e+e - pair mass is used to
obtain sin2θefflept, the effective leptonic determination
of the electroweak-mixing parameter sin2θW. The measurement
sample, recorded by the Collider Detector at Fermilab (CDF),
corresponds to 9.4 fb-1 of integrated luminosity from pp
collisions at a center-of-momentum energy of 1.96 TeV, and
is the full CDF Run II data set. The value of sin2θefflept
is found to be 0.23248±0.00053. The combination with the
previous CDF measurement based on μ+μ- pairs yields
sin2θefflept=0.23221±0.00046. This result, when
interpreted within the specified context of the standard
model assuming sin2θW=1-MW2/MZ2 and that the W- and Z-boson
masses are on-shell, yields sin2θW=0.22400±0.00045, or
equivalently a W-boson mass of 80.328±0.024
GeV/c2.},
Doi = {10.1103/PhysRevD.93.112016},
Key = {fds321122}
}
@article{fds358461,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Bella, LA and Arabidze, G},
Title = {Measurement of single top-quark production in association
with a W boson in the single-lepton channel at √s=8TeV
with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {8},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09371-7},
Abstract = {The production cross-section of a top quark in association
with a W boson is measured using proton–proton collisions
at s=8TeV. The dataset corresponds to an integrated
luminosity of 20.2fb-1, and was collected in 2012 by the
ATLAS detector at the Large Hadron Collider at CERN. The
analysis is performed in the single-lepton channel. Events
are selected by requiring one isolated lepton (electron or
muon) and at least three jets. A neural network is trained
to separate the tW signal from the dominant tt¯ background.
The cross-section is extracted from a binned profile
maximum-likelihood fit to a two-dimensional discriminant
built from the neural-network output and the invariant mass
of the hadronically decaying W boson. The measured
cross-section is σtW=26±7pb, in good agreement with the
Standard Model expectation.},
Doi = {10.1140/epjc/s10052-021-09371-7},
Key = {fds358461}
}
@article{fds349430,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
Title = {Measurement of soft-drop jet observables in pp collisions
with the ATLAS detector at s =13 TeV},
Journal = {Physical Review D},
Volume = {101},
Number = {5},
Year = {2020},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.101.052007},
Abstract = {Jet substructure quantities are measured using jets groomed
with the soft-drop grooming procedure in dijet events from
32.9 fb-1 of pp collisions collected with the ATLAS detector
at s=13 TeV. These observables are sensitive to a wide range
of QCD phenomena. Some observables, such as the jet mass and
opening angle between the two subjets which pass the
soft-drop condition, can be described by a high-order
(resummed) series in the strong coupling constant αS. Other
observables, such as the momentum sharing between the two
subjets, are nearly independent of αS. These observables
can be constructed using all interacting particles or using
only charged particles reconstructed in the inner tracking
detectors. Track-based versions of these observables are not
collinear safe, but are measured more precisely, and
universal nonperturbative functions can absorb the collinear
singularities. The unfolded data are directly compared with
QCD calculations and hadron-level Monte Carlo simulations.
The measurements are performed in different pseudorapidity
regions, which are then used to extract quark and gluon jet
shapes using the predicted quark and gluon fractions in each
region. All of the parton shower and analytical calculations
provide an excellent description of the data in most regions
of phase space.},
Doi = {10.1103/PhysRevD.101.052007},
Key = {fds349430}
}
@article{fds310291,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli,
F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak,
L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi,
M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov,
AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T},
Title = {Measurement of spin correlation in top-antitop quark events
and search for top squark pair production in pp collisions
at √s=8 TeV using the ATLAS detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {14},
Pages = {142001},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.114.142001},
Abstract = {A measurement of spin correlation in tt[over ¯] production
is presented using data collected with the ATLAS detector at
the Large Hadron Collider in proton-proton collisions at a
center-of-mass energy of 8 TeV, corresponding to an
integrated luminosity of 20.3 fb^{-1}. The correlation
between the top and antitop quark spins is extracted from
dilepton tt[over ¯] events by using the difference in the
azimuthal angle between the two charged leptons in the
laboratory frame. In the helicity basis the measured degree
of correlation corresponds to A_{helicity}=0.38±0.04, in
agreement with the standard model prediction. A search is
performed for pair production of top squarks with masses
close to the top quark mass decaying to predominantly
right-handed top quarks and a light neutralino, the lightest
supersymmetric particle. Top squarks with masses between the
top quark mass and 191 GeV are excluded at the 95%
confidence level.},
Doi = {10.1103/physrevlett.114.142001},
Key = {fds310291}
}
@article{fds372391,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Ahmadov, F and Agaras, MN and Bosman,
M},
Title = {Measurement of substructure-dependent jet suppression in
Pb+Pb collisions at 5.02 TeV with the ATLAS
detector},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054909},
Abstract = {The ATLAS detector at the Large Hadron Collider has been
used to measure jet substructure modification and
suppression in Pb+Pb collisions at a nucleon–nucleon
center-of-mass energy √sNN = 5.02 TeV in comparison with
proton–proton (pp) collisions at √s = 5.02 TeV. The
Pb+Pb data, collected in 2018, have an integrated luminosity
of 1.72 nb−1, while the ppdata, collected in 2017, have an
integrated luminosity of 260 pb−1. Jets used in this
analysis are clustered using the anti-kt algorithm with a
radius parameter R = 0.4. The jet constituents, defined by
both tracking and calorimeter information, are used to
determine the angular scale rg of the first hard splitting
inside the jet by reclustering them using the
Cambridge–Aachen algorithm and employing the soft-drop
grooming technique. The nuclear modification factor, RAA,
used to characterize jet suppression in Pb+Pb collisions, is
presented differentially in rg, jet transverse momentum, and
in intervals of collision centrality. The RAA value is
observed to depend significantly on jet rg. Jets produced
with the largest measured rg are found to be twice as
suppressed as those with the smallest rg in central Pb+Pb
collisions. The RAA values do not exhibit a strong variation
with jet pT in any of the rg intervals. The rg and pT
dependence of jet RAA is qualitatively consistent with a
picture of jet quenching arising from coherence and provides
the most direct evidence in support of this
approach.},
Doi = {10.1103/PhysRevC.107.054909},
Key = {fds372391}
}
@article{fds373907,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai,
K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos,
R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron
Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga,
D and Bauce, M and Bauer, P and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli,
M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul,
A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman,
M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger,
D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko,
D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
JWS and Carter, TM and Casado, MP and Casha, AF and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen,
A and Chen, B and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ and Clavijo
Columbie, JM and Clawson, SE and Clement, C and Clercx, J and Clissa, L and Coadou, Y and Cobal, M and Coccaro, A and Barrue, RFC and Coelho Lopes
De Sa and R},
Title = {Measurement of Suppression of Large-Radius Jets and Its
Dependence on Substructure in Pb+Pb Collisions at
sqrt[s_{NN}]=5.02 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {17},
Pages = {172301},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.172301},
Abstract = {This letter presents a measurement of the nuclear
modification factor of large-radius jets in
sqrt[s_{NN}]=5.02 TeV Pb+Pb collisions by the ATLAS
experiment. The measurement is performed using
1.72 nb^{-1} and 257 pb^{-1} of Pb+Pb and pp data,
respectively. The large-radius jets are reconstructed with
the anti-k_{t} algorithm using a radius parameter of R=1.0,
by reclustering anti-k_{t} R=0.2 jets, and are measured over
the transverse momentum (p_{T}) kinematic range of
158<p_{T}<1000 GeV and absolute pseudorapidity |y|<2.0.
The large-radius jet constituents are further reclustered
using the k_{t} algorithm in order to obtain the splitting
parameters, sqrt[d_{12}] and ΔR_{12}, which characterize
the transverse momentum scale and angular separation for the
hardest splitting in the jet, respectively. The nuclear
modification factor, R_{AA}, obtained by comparing the Pb+Pb
jet yields to those in pp collisions, is measured as a
function of jet transverse momentum (p_{T}) and sqrt[d_{12}]
or ΔR_{12}. A significant difference in the quenching of
large-radius jets having single subjet and those with more
complex substructure is observed. Systematic comparison of
jet suppression in terms of R_{AA} for different jet
definitions is also provided. Presented results support the
hypothesis that jets with hard internal splittings lose more
energy through quenching and provide a new perspective for
understanding the role of jet structure in jet
suppression.},
Doi = {10.1103/physrevlett.131.172301},
Key = {fds373907}
}
@article{fds308068,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $p \bar{p} \to t \bar{t}$ production
cross- section and the top quark mass at $\sqrt{s}$ = 1.96-
TeV in the all-hadronic decay mode},
Journal = {Phys. Rev.},
Volume = {D76},
Number = {7},
Pages = {072009},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.76.072009},
Abstract = {We report the measurements of the t[overline t] production
cross section and of the top quark mass using 1.02 fb-1 of
p[overline p] data collected with the CDF II detector at the
Fermilab Tevatron. We select events with six or more jets on
which a number of kinematical requirements are imposed by
means of a neural network algorithm. At least one of these
jets must be identified as initiated by a b-quark candidate
by the reconstruction of a secondary vertex. The cross
section is measured to be sigmat[overline
t]=8.3$\pm$1.0(stat)-1.5+2.0(syst)$\pm$0.5(lumi) pb, which
is consistent with the standard model prediction. The top
quark mass of 174.0$\pm$2.2(stat)$\pm$4.8(syst) GeV/c2 is
derived from a likelihood fit incorporating reconstructed
mass distributions representative of signal and
background.},
Doi = {10.1103/PhysRevD.76.072009},
Key = {fds308068}
}
@article{fds307915,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $t \bar{t}$ Production Cross Section in
$p \bar{p}$ Collisions at $\sqrt{s} = 1.96$ TeV using Soft
Electron $b$-Tagging},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.092002},
Abstract = {http://arxiv.org/abs/1002.3783},
Doi = {10.1103/PhysRevD.81.092002},
Key = {fds307915}
}
@article{fds308095,
Author = {Abulencia, and A, and others},
Title = {Measurement of the $t\bar{t}$ production cross section in
$p\bar{p}$ collisions at $\sqrt{s} = 1.96$ TeV using missing
$E_t$ + jets events with secondary vertex $b-
$tagging},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {20},
Pages = {202002},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.202002},
Abstract = {We present a measurement of the tt-bar production cross
section in p anti-p collisions at s**(1/2) = 1.96 TeV which
uses events with an inclusive signature of significant
missing transverse energy and jets. This is the first
measurement which makes no explicit lepton identification
requirements, so that sensitivity to W --> tau nu decays is
maintained. Heavy flavor jets from top quark decay are
identified with a secondary vertex tagging algorithm. From
311 pb-1 of data collected by the Collider Detector at
Fermilab we measure a production cross section of 5.8 +/-
1.2(stat.)+0.9_-0.7(syst.) pb for a top quark mass of 178
GeV/c2, in agreement with previous determinations and
standard model predictions.},
Doi = {10.1103/physrevlett.96.202002},
Key = {fds308095}
}
@article{fds307879,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the $t\overline{t}$ production cross section
in $p\overline{p}$ collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$
using events with large missing transverse energy and
jets},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {3},
Pages = {032003},
Publisher = {American Physical Society},
Year = {2011},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.84.032003},
Abstract = {In this paper we report a measurement of the tt̄ production
cross section in pp̄ collisions at √s=1.96TeV using data
corresponding to an integrated luminosity of 2.2fb-1
collected with the CDF II detector at the Tevatron
accelerator. We select events with significant missing
transverse energy and high jet multiplicity. This
measurement vetoes the presence of explicitly identified
electrons and muons, thus enhancing the tau contribution of
tt̄ decays. Signal events are discriminated from the
background using a neural network, and heavy flavor jets are
identified by a secondary-vertex tagging algorithm. We
measure a tt̄ production cross section of
7.99±0.55(stat)±0.76(syst)±0.46(lumi) pb, assuming a top
mass mtop=172.5GeV/c2, in agreement with previous
measurements and standard model predictions. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.84.032003},
Key = {fds307879}
}
@article{fds307874,
Author = {Aaltonen, and and, T and al, E},
Title = {Measurement of the $t\overline{t}$ production cross section
with an \textit{in~situ} calibration of $b$-jet
identification efficiency},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {7},
Pages = {071102},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.83.071102},
Abstract = {A measurement of the top-quark pair-production cross section
in pp̄ collisions at √s=1.96TeV using data corresponding
to an integrated luminosity of 1.12fb-1 collected with the
Collider Detector at Fermilab is presented. Decays of
top-quark pairs into the final states eν+ jets and μν+
jets are selected, and the cross section and the b-jet
identification efficiency are determined using a new
measurement technique which requires agreement between the
measured cross sections with exactly one and with multiple
identified b quarks from the top-quark decays. Assuming a
top-quark mass of 175GeV/c2, a cross section of
8.5±0.6(stat)±0. 7(syst)pb is measured. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.83.071102},
Key = {fds307874}
}
@article{fds307934,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $WW+WZ$ production cross section using a
matrix element technique in $lepton+jets$
events},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {11},
Pages = {112001},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.82.112001},
Abstract = {We present a measurement of the WW+WZ production cross
section observed in a final state consisting of an
identified electron or muon, two jets, and missing
transverse energy. The measurement is carried out in a data
sample corresponding to up to 4.6fb⊃-1 of integrated
luminosity at √s=1.96TeV collected by the CDF II detector.
Matrix element calculations are used to separate the diboson
signal from the large backgrounds. The WW+WZ cross section
is measured to be 17.4±3.3pb in agreement with standard
model predictions. A fit to the dijet invariant mass
spectrum yields a compatible cross section measurement. ©
2010 The American Physical Society.},
Doi = {10.1103/PhysRevD.82.112001},
Key = {fds307934}
}
@article{fds307909,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $WW+WZ$ Production Cross Section Using
the Lepton+Jets Final State at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {10},
Pages = {101801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.101801},
Abstract = {http://arxiv.org/abs/0911.4449},
Doi = {10.1103/PhysRevLett.104.101801},
Key = {fds307909}
}
@article{fds307904,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $W^+W^-$ Production Cross Section and
Search for Anomalous $WW\gamma$ and $WWZ$ Couplings in $p
\bar p$ Collisions at $\sqrt{s} = 1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {20},
Pages = {201801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.201801},
Abstract = {http://arxiv.org/abs/0912.4500},
Doi = {10.1103/PhysRevLett.104.201801},
Key = {fds307904}
}
@article{fds307908,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the $\Lambda_b$ Lifetime in $\Lambda_b \to
\Lambda_c^+ \pi^-$ Decays in $p\bar{p}$ Collisions at
$\sqrt{s} = 1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {10},
Pages = {102002},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.102002},
Abstract = {http://arxiv.org/abs/0912.3566},
Doi = {10.1103/PhysRevLett.104.102002},
Key = {fds307908}
}
@article{fds307868,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the ${B}^{-}$ lifetime using a simulation
free approach for trigger bias correction},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {3},
Pages = {032008},
Publisher = {American Physical Society},
Year = {2011},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.83.032008},
Abstract = {The collection of a large number of B-hadron decays to
hadronic final states at the CDF II Detector is possible due
to the presence of a trigger that selects events based on
track impact parameters. However, the nature of the
selection requirements of the trigger introduces a large
bias in the observed proper-decay-time distribution. A
lifetime measurement must correct for this bias, and the
conventional approach has been to use a Monte Carlo
simulation. The leading sources of systematic uncertainty in
the conventional approach are due to differences between the
data and the Monte Carlo simulation. In this paper, we
present an analytic method for bias correction without using
simulation, thereby removing any uncertainty due to the
differences between data and simulation. This method is
presented in the form of a measurement of the lifetime of
the B- using the mode B-→D0π -. The B- lifetime is
measured as τB -=1.663±0.023±0.015ps, where the first
uncertainty is statistical and the second systematic. This
new method results in a smaller systematic uncertainty in
comparison to methods that use simulation to correct for the
trigger bias. © 2011 American Physical Society.},
Doi = {10.1103/PhysRevD.83.032008},
Key = {fds307868}
}
@article{fds347498,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho,
J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Measurement of the W boson polarisation in [Formula:
see text] events from pp collisions at [Formula: see
text] = 8 TeV in the lepton + jets channel with
ATLAS.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {4},
Pages = {264},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4819-4},
Abstract = {This paper presents a measurement of the polarisation of
<i>W</i> bosons from [Formula: see text] decays,
reconstructed in events with one high-[Formula: see text]
lepton and at least four jets. Data from <i>pp</i>
collisions at the LHC were collected at [Formula: see text]
= 8 TeV and correspond to an integrated luminosity of
20.2 fb[Formula: see text]. The angle [Formula: see text]
between the <i>b</i>-quark from the top quark decay and a
direct <i>W</i> boson decay product in the <i>W</i> boson
rest frame is sensitive to the <i>W</i> boson polarisation.
Two different <i>W</i> decay products are used as
polarisation analysers: the charged lepton and the down-type
quark for the leptonically and hadronically decaying
<i>W</i> boson, respectively. The most precise measurement
of the <i>W</i> boson polarisation via the distribution of
[Formula: see text] is obtained using the leptonic analyser
and events in which at least two of the jets are tagged as
<i>b</i>-quark jets. The fitted fractions of longitudinal,
left- and right-handed polarisation states are [Formula: see
text], [Formula: see text] and [Formula: see text], and are
the most precisely measured <i>W</i> boson polarisation
fractions to date. Limits on anomalous couplings of the
<i>Wtb</i> vertex are set.},
Doi = {10.1140/epjc/s10052-017-4819-4},
Key = {fds347498}
}
@article{fds347466,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Biebel, O and Biedermann, D and Bianco, M and Bielski,
R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado,
MP and Casolino, M and Casper, DW and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
MR},
Title = {Measurement of the W-boson mass in pp collisions at s
= 7 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {2},
Pages = {110},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5475-4},
Abstract = {A measurement of the mass of the <i>W</i> boson is presented
based on proton-proton collision data recorded in 2011 at a
centre-of-mass energy of 7 TeV with the ATLAS detector at
the LHC, and corresponding to 4.6 fb - 1 of integrated
luminosity. The selected data sample consists of 7.8 × 10 6
candidates in the W → μ ν channel and 5.9 × 10 6
candidates in the W → e ν channel. The <i>W</i>-boson
mass is obtained from template fits to the reconstructed
distributions of the charged lepton transverse momentum and
of the <i>W</i> boson transverse mass in the electron and
muon decay channels, yielding m W = 80370 ± 7 ( stat. ) ±
11 ( exp. syst. ) ± 14 ( mod. syst. ) MeV = 80370 ± 19 MeV
, where the first uncertainty is statistical, the second
corresponds to the experimental systematic uncertainty, and
the third to the physics-modelling systematic uncertainty. A
measurement of the mass difference between the W + and W -
bosons yields m W + - m W - = - 29 ± 28
MeV.},
Doi = {10.1140/epjc/s10052-017-5475-4},
Key = {fds347466}
}
@article{fds321113,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Measurement of the angular coefficients in Z-boson events
using electron and muon pairs from data taken at √s = 8
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)159},
Abstract = {The angular distributions of Drell-Yan charged lepton pairs
in the vicinity of the Z-boson mass peak probe the
underlying QCD dynamics of Z-boson production. This paper
presents a measurement of the complete set of angular
coefficients A0−7 describing these distributions in the
Z-boson Collins-Soper frame. The data analysed correspond to
20.3 fb−1 of pp collisions at s=8 TeV, collected by the
ATLAS detector at the CERN LHC. The measurements are
compared to the most precise fixed-order calculations
currently available (O(αs2)) and with theoretical
predictions embedded in Monte Carlo generators. The
measurements are precise enough to probe QCD corrections
beyond the formal accuracy of these calculations and to
provide discrimination between different parton-shower
models. A significant deviation from the (O(αs2))
predictions is observed for A0 − A2. Evidence is found for
non-zero A5,6,7, consistent with expectations.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP08(2016)159},
Key = {fds321113}
}
@article{fds332356,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada,
J},
Title = {Measurement of the angular distribution of electrons from
[Formula Presented] decays observed in [Formula Presented]
collisions at [Formula Presented] TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {63},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2001},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.63.072001},
Abstract = {We present the first measurement of the electron angular
distribution parameter [Formula Presented] in [Formula
Presented] events produced in proton-antiproton collisions
as a function of the W boson transverse momentum. Our
analysis is based on data collected using the DØ detector
during the 1994–1995 Fermilab Tevatron run. We compare our
results with next-to-leading order perturbative QCD, which
predicts an angular distribution of [Formula Presented]
where [Formula Presented] is the polar angle of the electron
in the Collins-Soper frame. In the presence of QCD
corrections, the parameters [Formula Presented] and [Formula
Presented] become functions of [Formula Presented] the W
boson transverse momentum. This measurement provides a test
of next-to-leading order QCD corrections which are a
non-negligible contribution to the W boson mass measurement.
© 2001 The American Physical Society.},
Doi = {10.1103/PhysRevD.63.072001},
Key = {fds332356}
}
@article{fds308088,
Author = {Collaboration, CDF},
Title = {Measurement of the Associated ƒ× + ƒÝ„b Production
Cross Section in pp Collisions at = 1.8 TeV},
Journal = {Phys. Rev.},
Volume = {D60},
Number = {8},
Pages = {092003},
Year = {1999},
url = {http://dx.doi.org/10.1103/physrevlett.97.082004},
Abstract = {We present a measurement of the top quark pair production
cross section in pp collisions at square root of s = 1.96
TeV using 318 pb(-1) of data collected with the Collider
Detector at Fermilab. We select tt[over ] decays into the
final states enu+jets and mu nu+ jets, in which at least one
b quark from the t-quark decays is identified using a
secondary vertex-finding algorithm. Assuming a top quark
mass of 178 GeV/c2, we measure a cross section of 8.7 +/-
0.9(stat)(-0.9)+1.1(syst) pb. We also report the first
observation of tt[over ] with significance greater than
5sigma in the subsample in which both b quarks are
identified, corresponding to a cross section of
10.1(-1.4)+1.6(stat)(-1.3)+2.0(syst) pb.},
Doi = {10.1103/physrevlett.97.082004},
Key = {fds308088}
}
@article{fds307568,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau,
M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
RN},
Title = {Measurement of the azimuthal angle dependence of inclusive
jet yields in Pb+Pb collisions at √(sNN)=2.76 TeV with the
ATLAS detector.},
Journal = {Physical review letters},
Volume = {111},
Number = {15},
Pages = {152301},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.111.152301},
Abstract = {Measurements of the variation of inclusive jet suppression
as a function of relative azimuthal angle, Δφ, with
respect to the elliptic event plane provide insight into the
path-length dependence of jet quenching. ATLAS has measured
the Δφ dependence of jet yields in 0.14 nb(-1) of
√(s(NN))=2.76 TeV Pb+Pb collisions at the LHC for jet
transverse momenta p(T)>45 GeV in different collision
centrality bins using an underlying event subtraction
procedure that accounts for elliptic flow. The variation of
the jet yield with Δφ was characterized by the parameter,
v(2)(jet), and the ratio of out-of-plane (Δφ~π/2) to
in-plane (Δφ~0) yields. Nonzero v(2)(jet) values were
measured in all centrality bins for p(T)<160 GeV. The jet
yields are observed to vary by as much as 20% between
in-plane and out-of-plane directions.},
Doi = {10.1103/physrevlett.111.152301},
Key = {fds307568}
}
@article{fds310404,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abou
Zeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amor’Os, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Measurement of the azimuthal anisotropy for charged particle
production in √SNN = 2.76 TeV lead-lead
collisions with the ATLAS detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {86},
Number = {1},
Pages = {014907-1-014907-41},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevC.86.014907},
Abstract = {Differential measurements of charged particle azimuthal
anisotropy are presented for lead-lead collisions at √sNN
= 2.76 TeV with the ATLAS detector at the LHC, based on an
integrated luminosity of approximately 8 μb− 1. This
anisotropy is characterized via a Fourier expansion of the
distribution of charged particles in azimuthal angle
relative to the reaction plane, with the coefficients vn
denoting the magnitude of the anisotropy. Significant
v2–v6 values are obtained as a function of transverse
momentum (0.5 < pT < 20 GeV), pseudorapidity (|η| < 2.5),
and centrality using an event plane method. The vn values
for n ≥ 3 are found to vary weakly with both η and
centrality, and their pT dependencies are found to follow an
approximate scaling relation, v1/nn (pT) ∝ v1/22 (pT),
except in the top 5% most central collisions. A Fourier
analysis of the charged particle pair distribution in
relative azimuthal angle (Δϕ = ϕa − ϕb) is performed
to extract the coefficients vn, n = (cos nΔϕ). For pairs
of charged particles with a large pseudorapidity gap (|Δη
= ηa − ηb| > 2) and one particle with pT < 3 GeV, the
v2,2–v6,6 values are found to factorize as vn, n(paT, pbT)
≈ vn(paT)vn(pbT) in central and midcentral events. Such
factorization suggests that these values of v2,2–v6,6 are
primarily attributable to the response of the created matter
to the fluctuations in the geometry of the initial state. A
detailed study shows that the v1,1(paT, pbT) data are
consistent with the combined contributions from a
rapidity-even v1 and global momentum conservation.A
two-component fit is used to extract the v1 contribution.
The extracted v1 isobserved to cross zero at pT ≈ 1.0 GeV,
reaches a maximum at 4–5 GeV with a value comparable to
that for v3, and decreases at higher pT.},
Doi = {10.1103/PhysRevC.86.014907},
Key = {fds310404}
}
@article{fds347485,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V},
Title = {Measurement of the azimuthal anisotropy of charged particles
produced in s NN = 5.02 TeV Pb+Pb collisions with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {12},
Pages = {997},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6468-7},
Abstract = {Measurements of the azimuthal anisotropy in lead-lead
collisions at s NN = 5.02 TeV are presented using a data
sample corresponding to 0.49 nb - 1 integrated luminosity
collected by the ATLAS experiment at the LHC in 2015. The
recorded minimum-bias sample is enhanced by triggers for
"ultra-central" collisions, providing an opportunity to
perform detailed study of flow harmonics in the regime where
the initial state is dominated by fluctuations. The
anisotropy of the charged-particle azimuthal angle
distributions is characterized by the Fourier coefficients,
v 2 - v 7 , which are measured using the two-particle
correlation, scalar-product and event-plane methods. The
goal of the paper is to provide measurements of the
differential as well as integrated flow harmonics v n over
wide ranges of the transverse momentum, 0.5 < p T <
60 GeV, the pseudorapidity, | η | < 2.5, and the
collision centrality 0-80%. Results from different methods
are compared and discussed in the context of previous and
recent measurements in Pb+Pb collisions at s NN = 2.76
TeV and 5.02 TeV . In particular, the shape of the p T
dependence of elliptic or triangular flow harmonics is
observed to be very similar at different centralities after
scaling the v n and p T values by constant factors over the
centrality interval 0-60% and the p T range 0.5 < p T <
5 GeV.},
Doi = {10.1140/epjc/s10052-018-6468-7},
Key = {fds347485}
}
@article{fds349434,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA},
Title = {Measurement of the azimuthal anisotropy of charged-particle
production in Xe+Xe collisions at sNN =5.44 TeV with the
ATLAS detector},
Journal = {Physical Review C},
Volume = {101},
Number = {2},
Year = {2020},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevC.101.024906},
Abstract = {This paper describes the measurements of flow harmonics
v2-v6 in 3μb-1 of Xe+Xe collisions at sNN=5.44 TeV
performed using the ATLAS detector at the Large Hadron
Collider (LHC). Measurements of the centrality,
multiplicity, and pT dependence of the vn obtained using
two-particle correlations and the scalar product technique
are presented. The measurements are also performed using a
template-fit procedure, which was developed to remove
nonflow correlations in small collision systems. This
nonflow removal is shown to have a significant influence on
the measured vn at high pT, especially in peripheral events.
Comparisons of the measured vn with measurements in Pb+Pb
collisions and p+Pb collisions at sNN=5.02 TeV are also
presented. The vn values in Xe+Xe collisions are observed to
be larger than those in Pb+Pb collisions for n=2, 3, and 4
in the most central events. However, with decreasing
centrality or increasing harmonic order n, the vn values in
Xe+Xe collisions become smaller than those in Pb+Pb
collisions. The vn in Xe+Xe and Pb+Pb collisions are also
compared as a function of the mean number of participating
nucleons, (Npart), and the measured charged-particle
multiplicity in the detector. The v3 values in Xe+Xe and
Pb+Pb collisions are observed to be similar at the same
(Npart) or multiplicity, but the other harmonics are
significantly different. The ratios of the measured vn in
Xe+Xe and Pb+Pb collisions, as a function of centrality, are
also compared to theoretical calculations.},
Doi = {10.1103/PhysRevC.101.024906},
Key = {fds349434}
}
@article{fds307737,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the azimuthal ordering of charged hadrons
with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.86.052005},
Abstract = {This paper presents a study of the possible ordering of
charged hadrons in the azimuthal angle relative to the beam
axis in high-energy proton-proton collisions at the Large
Hadron Collider (LHC). A spectral analysis of correlations
between longitudinal and transverse components of the
momentum of the charged hadrons, driven by the search for
phenomena related to the structure of the QCD field, is
performed. Data were recorded with the ATLAS detector at
center-of-mass energies of √s=900GeV and √s=7TeV. The
correlations measured in a kinematic region dominated by
low-pT particles are not well described by conventional
models of hadron production. The measured spectra show
features consistent with the fragmentation of a QCD string
represented by a helixlike ordered gluon chain. © 2012
CERN.},
Doi = {10.1103/PhysRevD.86.052005},
Key = {fds307737}
}
@article{fds308126,
Author = {Abulencia, and A, and others},
Title = {Measurement of the b jet cross section in events with a Z
boson in $p\bar{p}$ collisions at $\sqrt{s} =$
1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D74},
Number = {3},
Pages = {032008},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.032008},
Abstract = {A measurement of the inclusive bottom jet cross section is
presented for events containing a Z boson in p anti-p
collisions at s**(1/2) = 1.96 TeV using the Collider
Detector at Fermilab. Z bosons are identified in their
electron and muon decay modes, and b jets with E(t) > 20 GeV
and |eta| l+ l-) = 0.93 +/- 0.36 pb is found, where B(Z -->
l+ l-) is the branching ratio of the Z boson or gamma* into
a single flavor dilepton pair (e or mu) in the mass range
between 66 and 116 GeV/c2. The ratio of b jets to the total
number of jets of any flavor in the Z sample, within the
same kinematic range as the b jets, is 2.36 +/- 0.92\%.
Here, the uncertainties are the quadratic sum of statistical
and systematic uncertainties. Predictions made with NLO QCD
agree, within experimental and theoretical uncertainties,
with these measurements.},
Doi = {10.1103/PhysRevD.74.032008},
Key = {fds308126}
}
@article{fds307827,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
M and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, H-C and Farrington, S and Feindt,
M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan,
N and Redondo, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T},
Title = {Measurement of the B(s)0 lifetime in fully and partially
reconstructed B(s)0→D(s)(-)(ϕπ(-))X decays in p¯p
collisions at √s=1.96 TeV.},
Journal = {Physical review letters},
Volume = {107},
Number = {27},
Pages = {272001},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.107.272001},
Abstract = {We present a measurement of the B(s)(0) lifetime in fully
and partially reconstructed B(s)(0)→D(s)(-)(ϕπ(-))X
decays in 1.3 fb(-1) collected in pp ¯ collisions at
√s=1.96 TeV by the CDF II detector at the Fermilab
Tevatron. We measure τ(B(s)(0))=1.518±0.041(stat)±0.027(syst) ps.
The ratio of this result and the world average B(0) lifetime
yields τ(B(s)(0))/τ(B(0))=0.99±0.03, which is in
agreement with recent theoretical predictions.},
Doi = {10.1103/physrevlett.107.272001},
Key = {fds307827}
}
@article{fds308079,
Author = {Abulencia, and A, and others},
Title = {Measurement of the B+ production cross section in p anti-p
collisions at s**(1/2) = 1960-GeV},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {5},
Pages = {012010},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.93.052001},
Abstract = {We present a new measurement of the B+ meson differential
cross section dsigma/dpT at sqrt(s)=1960 GeV. The data
correspond to an integrated luminosity of 739 pb-1 collected
with the upgraded CDF detector (CDF II) at the Fermilab
Tevatron collider. B+ candidates are reconstructed through
the decay B+-->J/psiK+, with J/psi-->µ+µ-. The integrated
cross section for producing B+ mesons with pT>=6 GeV/c and
|y|},
Doi = {10.1103/PhysRevD.93.052001},
Key = {fds308079}
}
@article{fds307787,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
NJ and Collins-Tooth, C and Collot, J},
Title = {Measurement of the b-hadron production cross section using
decays to D *+μ -X final states in pp
collisions at √s = 7 TeV with the ATLAS
detector},
Journal = {Nuclear Physics B},
Volume = {864},
Number = {3},
Pages = {341-381},
Publisher = {Elsevier BV},
Year = {2012},
url = {http://dx.doi.org/10.1016/j.nuclphysb.2012.07.009},
Abstract = {The b-hadron production cross section is measured with the
ATLAS detector in pp collisions at s=7TeV, using 3.3pb -1 of
integrated luminosity, collected during the 2010 LHC run.
The b-hadrons are selected by partially reconstructing D
z.ast;+μ -X final states. Differential cross sections are
measured as functions of the transverse momentum and
pseudorapidity. The measured production cross section for a
b-hadron with p T>9GeV and |n|<2.5 is
32.7±0.8(stat.)-6.8+4.5(syst.)μb, higher than the
next-to-leading-order QCD predictions but consistent within
the experimental and theoretical uncertainties. ©
2012.},
Doi = {10.1016/j.nuclphysb.2012.07.009},
Key = {fds307787}
}
@article{fds307987,
Author = {Aaltonen, T and others},
Title = {Measurement of the b-hadron production cross section using
decays to mu[sup -]D[sup 0]X final states in p[overline p]
collisions at sqrt(s) = 1.96 TeV},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {9},
Pages = {092003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.092003},
Abstract = {We report a measurement of the production cross section for
b hadrons in pp̄ collisions at s=1.96TeV. Using a data
sample derived from an integrated luminosity of 83pb-1
collected with the upgraded Collider Detector (CDF II) at
the Fermilab Tevatron, we analyze b hadrons, Hb, partially
reconstructed in the semileptonic decay mode Hb→μ-D0X.
Our measurement of the inclusive production cross section
for b hadrons with transverse momentum pT>9GeV/c and
rapidity |y|<0.6 is σ=1.30μb±0.05μb(stat)±0.
14μb(syst)±0.07μb(B), where the uncertainties are
statistical, systematic, and from branching fractions,
respectively. The differential cross sections dσ/dpT are
found to be in good agreement with recent measurements of
the Hb cross section and well described by fixed-order
next-to-leading logarithm predictions. © 2009 The American
Physical Society.},
Doi = {10.1103/PhysRevD.79.092003},
Key = {fds307987}
}
@article{fds361246,
Author = {Abulencia, and A, and others},
Title = {Measurement of the B/s0 anti-B/s0 oscillation
frequency},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {191802},
Pages = {062003},
Year = {2006},
Abstract = {We measure the masses of $b$ hadrons in exclusively
reconstructed final states containing a $J/\psi\to\mu^-\mu^+$
decay using $\rm 220 pb^{-1}$ of data collected by the CDF
II experiment. We find: m(B^+) = 5279.10 \pm 0.41_{(stat.)}
\pm 0.36_{(sys.)} MeVcc, m(B^0) = 5279.63 \pm 0.53_{(stat.)}
\pm 0.33_{(sys.)} MeVcc, m(B^0_s) = 5366.01 \pm
0.73_{(stat.)} \pm 0.33_{(sys.)} MeVcc, m(\Lambda^0_b) =
5619.7 \pm 1.2_{(stat.)} \pm 1.2_{(sys.)} MeVcc. m(B^+) -
m(B^0) = -0.53 \pm 0.67_{(stat.)} \pm 0.14_{(sys.)} MeVcc,
m(B^0_s) - m(B^0) = 86.38 \pm 0.90_{(stat.)} \pm
0.06_{(sys.)} MeVcc m(\Lambda^0_b) - m(B^0) = 339.2 \pm
1.4_{(stat.)} \pm 0.1_{(sys.)} MeVcc. The measurements of
the $B^0_s$, $\Lambda^0_b$ mass, $m(B^0_s)-m(B^0)$ and
$m(\Lambda^0_b)-m(B^0)$ mass difference are of better
precision than the current world averages.},
Key = {fds361246}
}
@article{fds362145,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and DiTuro, P and Dorr, C and Donati, S and Donega, M and Dong, P and Donini,
J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris, N and Giolo, K and Giordani, M and Giromini,
P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos,
G and Goncharov, M and Gonzalez, O and Gorelov, I and Goshaw, AT and Gotra,
Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Hahn, K and Halkiadakis,
E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer, A and Heinemann,
B and Heinrich, J and Herndon, M and Hidas, D and Hill, CS and Hirschbuehl,
D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi,
G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon,
T and Kang, J and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto,
A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mulmenstadt, J and Mukherjee, A and Muller, T and Mumford, R and Murat,
P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg,
K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou,
V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel,
NV and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli,
S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P},
Title = {Measurement of the Bc+ meson lifetime using the decay mode
Bc+→J/ψe+νe},
Journal = {Physical Review Letters},
Volume = {97},
Number = {1},
Pages = {012002},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevLett.97.012002},
Abstract = {We present a measurement of the Bc+ meson lifetime in the
decay mode Bc+→J/ψe+νe using the Collider Detector at
Fermilab II detector at the Fermilab Tevatron Collider. From
a sample of about 360pb-1 of pp̄ collisions at s=1.96TeV,
we reconstruct J/ψe+ pairs with invariant mass in the
kinematically allowed range 4<MJ/ψe<6GeV/c2. A fit to
the decay-length distribution of 238 signal events yields a
measured Bc+ meson lifetime of 0.463+0.073-0.065(stat)±0.036(syst)ps.
© 2006 The American Physical Society.},
Doi = {10.1103/PhysRevLett.97.012002},
Key = {fds362145}
}
@article{fds307641,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {Measurement of the Bc-meson lifetime in the decay
Bc-→J/ψπ},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.87.011101},
Abstract = {The lifetime of the Bc- meson is measured using 272
exclusive Bc-→J/ψ(→μ+μ-)π- decays reconstructed in
data from proton-antiproton collisions corresponding to an
integrated luminosity of 6.7 fb-1 recorded by the CDF II
detector at the Fermilab Tevatron. The lifetime of the Bc-
meson is measured to be τ(Bc-)=0.452±0.048(stat)±0.027(syst)
ps. This is the first measurement of the Bc- meson lifetime
in a fully reconstructed hadronic channel, and it agrees
with previous results and has comparable precision. © 2013
American Physical Society.},
Doi = {10.1103/PhysRevD.87.011101},
Key = {fds307641}
}
@article{fds307679,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grillo, L and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the bottom-strange meson mixing phase in the
full CDF data set.},
Journal = {Physical review letters},
Volume = {109},
Number = {17},
Pages = {171802},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.109.171802},
Abstract = {We report a measurement of the bottom-strange meson mixing
phase β(s) using the time evolution of B(s)(0)→J/ψ(→μ(+)μ(-))φ(→K(+)K(-))
decays in which the quark-flavor content of the
bottom-strange meson is identified at production. This
measurement uses the full data set of proton-antiproton
collisions at √s=1.96 TeV collected by the Collider
Detector experiment at the Fermilab Tevatron, corresponding
to 9.6 fb(-1) of integrated luminosity. We report confidence
regions in the two-dimensional space of β(s) and the
B(s)(0) decay-width difference ΔΓ(s) and measure
β(s)∈[-π/2,-1.51]∪[-0.06,0.30]∪[1.26,π/2] at the
68% confidence level, in agreement with the standard model
expectation. Assuming the standard model value of β(s), we
also determine ΔΓ(s)=0.068±0.026(stat)±0.009(syst)
ps(-1) and the mean B(s)(0) lifetime τ(s)=1.528±0.019(stat)±0.009(syst)
ps, which are consistent and competitive with determinations
by other experiments.},
Doi = {10.1103/physrevlett.109.171802},
Key = {fds307679}
}
@article{fds307817,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli,
M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F and D'errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan,
G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giakoumopoulou,
V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh,
SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Poukhov,
O and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Squillacioti, P and Stancari, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, WM and Yeh, GP and Yi, K and Yoh,
J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zucchelli, S},
Title = {Measurement of the branching fraction B(Λb0→Λc+π
-π +π -) at
CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.85.032003},
Abstract = {We report an analysis of the Λb0→Λc+π -π +π - decay
in a data sample collected by the CDF II detector at the
Fermilab Tevatron corresponding to 2.4fb -1 of integrated
luminosity. We reconstruct the currently largest samples of
the decay modes Λb0→Λ c(2595) +π - (with Λ c(2595)
+→Λc+π +π -), Λb0→Λ c(2625) +π - (with Λ c(2625)
+→Λc+π +π -), Λb0→Σ c(2455) ++π -π - (with Σ
c(2455) ++→Λc+π +), and Λb0→Σ c(2455)0π +π - (with
Σ c(2455)0→Λc+π -) and measure the branching fractions
relative to the Λb0→Λc+π - branching fraction. We
measure the ratio B(Λb0→Λc+π -π +π -)/B(Λb0→Λc+π
-)=3.04±0.33(stat)-0.55+0.70(syst) which is used to derive
B(Λb0→Λc+π -π +π -)= (26.8-11.2+11.9)×10 -3. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.032003},
Key = {fds307817}
}
@article{fds313605,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of the branching ratio Γ(Λb0→ψ(2S)Λ0)/Γ(Λb0→J/ψΛ0)
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {751},
Pages = {63-80},
Publisher = {Elsevier BV},
Year = {2015},
Month = {December},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2015.10.009},
Abstract = {An observation of the Λb0→ψ(2S)Λ0 decay and a
comparison of its branching fraction with that of the
Λb0→J/ψΛ0 decay has been made with the ATLAS detector
in proton–proton collisions at s=8 TeV at the LHC using an
integrated luminosity of 20.6 fb−1. The J/ψ and ψ(2S)
mesons are reconstructed in their decays to a muon pair,
while the Λ0→pπ− decay is exploited for the Λ0 baryon
reconstruction. The Λb0 baryons are reconstructed with
transverse momentum pT>10 GeV and pseudorapidity |η|<2.1.
The measured branching ratio of the Λb0→ψ(2S)Λ0 and
Λb0→J/ψΛ0 decays is Γ(Λb0→ψ(2S)Λ0)/Γ(Λb0→J/ψΛ0)=0.501±0.033(stat)±0.019(syst),
lower than the expectation from the covariant quark
model.},
Doi = {10.1016/j.physletb.2015.10.009},
Key = {fds313605}
}
@article{fds310394,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {Measurement of the centrality and pseudorapidity dependence
of the integrated elliptic flow in lead-lead collisions at
[Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {8},
Pages = {2982},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2982-4},
Abstract = {The integrated elliptic flow of charged particles produced
in Pb+Pb collisions at [Formula: see text] TeV has been
measured with the ATLAS detector using data collected at the
Large Hadron Collider. The anisotropy parameter, [Formula:
see text], was measured in the pseudorapidity range
[Formula: see text] with the event-plane method. In order to
include tracks with very low transverse momentum [Formula:
see text], thus reducing the uncertainty in [Formula: see
text] integrated over [Formula: see text], a [Formula: see
text] data sample recorded without a magnetic field in the
tracking detectors is used. The centrality dependence of the
integrated [Formula: see text] is compared to other
measurements obtained with higher [Formula: see text]
thresholds. The integrated elliptic flow is weakly
decreasing with [Formula: see text]. The integrated
[Formula: see text] transformed to the rest frame of one of
the colliding nuclei is compared to the lower-energy RHIC
data.},
Doi = {10.1140/epjc/s10052-014-2982-4},
Key = {fds310394}
}
@article{fds307764,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Measurement of the centrality dependence of the charged
particle pseudorapidity distribution in lead-lead collisions
at √s NN=2.76 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {710},
Number = {3},
Pages = {363-382},
Publisher = {Elsevier BV},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2012.02.045},
Abstract = {The ATLAS experiment at the LHC has measured the centrality
dependence of charged particle pseudorapidity distributions
over |η|<2 in lead-lead collisions at a nucleon-nucleon
centre-of-mass energy of √s NN=2.76 TeV. In order to
include particles with transverse momentum as low as 30 MeV,
the data were recorded with the central solenoid magnet off.
Charged particles were reconstructed with two algorithms
(2-point "tracklets" and full tracks) using information from
the pixel detector only. The lead-lead collision centrality
was characterized by the total transverse energy in the
forward calorimeter in the range 3.2<|η|<4.9. Measurements
are presented of the per-event charged particle
pseudorapidity distribution, dN ch/dη, and the average
charged particle multiplicity in the pseudorapidity interval
|η|<0.5 in several intervals of collision centrality. The
results are compared to previous mid-rapidity measurements
at the LHC and RHIC. The variation of the mid-rapidity
charged particle yield per colliding nucleon pair with the
number of participants is consistent with lower sNN results.
The shape of the dN ch/dη distribution is found to be
independent of centrality within the systematic
uncertainties of the measurement. © 2012
CERN.},
Doi = {10.1016/j.physletb.2012.02.045},
Key = {fds307764}
}
@article{fds315363,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, J-F and Argyropoulos,
S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
P and Balli, F and Banas, E and Banerjee, S and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho
Toro, R and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa,
A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavez
Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi,
IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Coggeshall, J and Cole, B and Cole, S and Colijn, AP and Collins-Tooth, C and Collot, J and Colombo,
T},
Title = {Measurement of the centrality dependence of the
charged-particle pseudorapidity distribution in proton-lead
collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {4},
Pages = {199},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4002-3},
Abstract = {The centrality dependence of the mean charged-particle
multiplicity as a function of pseudorapidity is measured in
approximately 1 [Formula: see text]b[Formula: see text] of
proton-lead collisions at a nucleon-nucleon centre-of-mass
energy of [Formula: see text] [Formula: see text] using the
ATLAS detector at the Large Hadron Collider. Charged
particles with absolute pseudorapidity less than 2.7 are
reconstructed using the ATLAS pixel detector. The [Formula:
see text] collision centrality is characterised by the total
transverse energy measured in the Pb-going direction of the
forward calorimeter. The charged-particle pseudorapidity
distributions are found to vary strongly with centrality,
with an increasing asymmetry between the proton-going and
Pb-going directions as the collisions become more central.
Three different estimations of the number of nucleons
participating in the [Formula: see text] collision have been
carried out using the Glauber model as well as two
Glauber-Gribov inspired extensions to the Glauber model.
Charged-particle multiplicities per participant pair are
found to vary differently for these three models,
highlighting the importance of including colour fluctuations
in nucleon-nucleon collisions in the modelling of the
initial state of [Formula: see text] collisions.},
Doi = {10.1140/epjc/s10052-016-4002-3},
Key = {fds315363}
}
@article{fds376310,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Aktas, S and Al Khoury and K and Alberghi,
GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Alegria, ZL and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arbiol Val and SJ and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling,
J-H and Arnaez, O and Arnold, H and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Baer, TM and Bagnaia, P and Bahmani, M and Bahner, D and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barel, MZ and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beaucamp, JY and Beauchemin, PH and Becherer, F and Bechtle, P and Beck,
HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berrocal Guardia and A and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhalla, NK and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos,
F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chakraborty, D and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Clark, A},
Title = {Measurement of the Centrality Dependence of the Dijet Yield
in p+Pb Collisions at sqrt[s_{NN}]=8.16 TeV with the
ATLAS Detector.},
Journal = {Physical review letters},
Volume = {132},
Number = {10},
Pages = {102301},
Year = {2024},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.132.102301},
Abstract = {ATLAS measured the centrality dependence of the dijet yield
using 165 nb^{-1} of p+Pb data collected at
sqrt[s_{NN}]=8.16 TeV in 2016. The event centrality,
which reflects the p+Pb impact parameter, is characterized
by the total transverse energy registered in the Pb-going
side of the forward calorimeter. The central-to-peripheral
ratio of the scaled dijet yields, R_{CP}, is evaluated, and
the results are presented as a function of variables that
reflect the kinematics of the initial hard parton scattering
process. The R_{CP} shows a scaling with the Bjorken x of
the parton originating from the proton, x_{p}, while no such
trend is observed as a function of x_{Pb}. This analysis
provides unique input to understanding the role of small
proton spatial configurations in p+Pb collisions by covering
parton momentum fractions from the valence region down to
x_{p}∼10^{-3} and x_{Pb}∼4×10^{-4}.},
Doi = {10.1103/physrevlett.132.102301},
Key = {fds376310}
}
@article{fds310286,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurement of the charge asymmetry in dileptonic decays of
top quark pairs in pp collisions at √s = 7 TeV using the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {5},
Publisher = {Springer Nature},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2015)061},
Abstract = {A measurement of the top-antitop (tt¯) charge asymmetry is
presented using data corresponding to an integrated
luminosity of 4.6 fb−1 of LHC pp collisions at a
centreof-mass energy of 7 TeV collected by the ATLAS
detector. Events with two charged leptons, at least two jets
and large missing transverse momentum are selected. Two
observables are studied: ACℓℓ based on the identified
charged leptons, and (Formula Presented.), based on the
reconstructed tt final state. The asymmetries are measured
to be (Formula Presented.). The measured values are in
agreement with the Standard Model predictions.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP05(2015)061},
Key = {fds310286}
}
@article{fds356770,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A},
Title = {Measurement of the charge asymmetry in highly boosted
top-quark pair production in √s=8 TeV pp collision data
collected by the ATLAS experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {756},
Pages = {52-71},
Year = {2016},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2016.02.055},
Abstract = {In the pp→tt¯ process the angular distributions of top
and anti-top quarks are expected to present a subtle
difference, which could be enhanced by processes not
included in the Standard Model. This Letter presents a
measurement of the charge asymmetry in events where the
top-quark pair is produced with a large invariant mass. The
analysis is performed on 20.3 fb−1 of pp collision data at
s=8TeV collected by the ATLAS experiment at the LHC, using
reconstruction techniques specifically designed for the
decay topology of highly boosted top quarks. The charge
asymmetry in a fiducial region with large invariant mass of
the top-quark pair (mtt¯>0.75 TeV) and an absolute rapidity
difference of the top and anti-top quark candidates within
−2<|yt|−|yt¯|<2 is measured to be 4.2±3.2%, in
agreement with the Standard Model prediction at
next-to-leading order. A differential measurement in three
tt¯ mass bins is also presented.},
Doi = {10.1016/j.physletb.2016.02.055},
Key = {fds356770}
}
@article{fds307729,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati,
S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
W},
Title = {Measurement of the charge asymmetry in top quark pair
production in pp collisions at [Formula: see text]
using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {72},
Number = {6},
Pages = {2039},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2039-5},
Abstract = {A measurement of the top-antitop production charge asymmetry
<i>A</i><sub><i>C</i></sub> is presented using data
corresponding to an integrated luminosity of 1.04
fb<sup>-1</sup> of <i>pp</i> collisions at [Formula: see
text] TeV collected by the ATLAS detector at the LHC.
Events are selected with a single lepton (electron or muon),
missing transverse momentum and at least four jets of which
at least one jet is identified as coming from a
<i>b</i>-quark. A kinematic fit is used to reconstruct the
[Formula: see text] event topology. After background
subtraction, a Bayesian unfolding procedure is performed to
correct for acceptance and detector effects. The measured
value of <i>A</i><sub><i>C</i></sub> is [Formula: see text],
consistent with the prediction from the MC@NLO Monte Carlo
generator of <i>A</i><sub><i>C</i></sub> =0.006±0.002.
Measurements of <i>A</i><sub><i>C</i></sub> in two ranges of
invariant mass of the top-antitop pair are also
shown.},
Doi = {10.1140/epjc/s10052-012-2039-5},
Key = {fds307729}
}
@article{fds372122,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V},
Title = {Measurement of the charge asymmetry in top-quark pair
production in association with a photon with the ATLAS
experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137848},
Abstract = {A measurement of the charge asymmetry in top-quark pair
(tt¯) production in association with a photon is presented.
The measurement is performed in the single-lepton tt¯ decay
channel using proton–proton collision data collected with
the ATLAS detector at the Large Hadron Collider at CERN at a
centre-of-mass-energy of 13 TeV during the years
2015–2018, corresponding to an integrated luminosity of
139 fb−1. The charge asymmetry is obtained from the
distribution of the difference of the absolute rapidities of
the top quark and antiquark using a profile likelihood
unfolding approach. It is measured to be AC=−0.003±0.029
in agreement with the Standard Model expectation.},
Doi = {10.1016/j.physletb.2023.137848},
Key = {fds372122}
}
@article{fds323672,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard,
CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Measurement of the charge asymmetry in top-quark pair
production in the lepton-plus-jets final state in pp
collision data at [Formula: see text] with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {87},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3910-6},
Abstract = {This paper reports inclusive and differential measurements
of the [Formula: see text] charge asymmetry [Formula: see
text] in [Formula: see text] of [Formula: see text][Formula:
see text] collisions recorded by the ATLAS experiment at the
Large Hadron Collider at CERN. Three differential
measurements are performed as a function of the invariant
mass, transverse momentum and longitudinal boost of the
[Formula: see text] system. The [Formula: see text] pairs
are selected in the single-lepton channels (<i>e</i> or
[Formula: see text]) with at least four jets, and a
likelihood fit is used to reconstruct the [Formula: see
text] event kinematics. A Bayesian unfolding procedure is
performed to infer the asymmetry at parton level from the
observed data distribution. The inclusive [Formula: see
text] charge asymmetry is measured to be [Formula: see text]
(stat. [Formula: see text] syst.). The inclusive and
differential measurements are compatible with the values
predicted by the Standard Model.},
Doi = {10.1140/epjc/s10052-016-3910-6},
Key = {fds323672}
}
@article{fds347519,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN},
Title = {Measurement of the charged-particle multiplicity inside jets
from [Formula: see text][Formula: see text] pp
collisions with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {6},
Pages = {322},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4126-5},
Abstract = {The number of charged particles inside jets is a widely used
discriminant for identifying the quark or gluon nature of
the initiating parton and is sensitive to both the
perturbative and non-perturbative components of
fragmentation. This paper presents a measurement of the
average number of charged particles with [Formula: see text]
[Formula: see text] inside high-momentum jets in dijet
events using 20.3 fb[Formula: see text] of data recorded
with the ATLAS detector in <i>pp</i> collisions at [Formula:
see text] [Formula: see text] collisions at the LHC. The
jets considered have transverse momenta from 50 [Formula:
see text] up to and beyond 1.5 [Formula: see text]. The
reconstructed charged-particle track multiplicity
distribution is unfolded to remove distortions from detector
effects and the resulting charged-particle multiplicity is
compared to several models. Furthermore, quark and gluon jet
fractions are used to extract the average charged-particle
multiplicity for quark and gluon jets separately.},
Doi = {10.1140/epjc/s10052-016-4126-5},
Key = {fds347519}
}
@article{fds313619,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Akesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of the correlation between flow harmonics of
different order in lead-lead collisions at √sNN
= 2.76 TeV with the ATLAS detector},
Journal = {Physical Review C - Nuclear Physics},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
ISSN = {0556-2813},
url = {http://dx.doi.org/10.1103/PhysRevC.92.034903},
Abstract = {Correlations between the elliptic or triangular flow
coefficients vm (m = 2 or 3) and other flow harmonics vn (n
= 2 to 5) are measured using √sNN = 2.76 TeV Pb + Pb
collision data collected in 2010 by the ATLAS experiment at
the LHC, corresponding to an integrated luminosity of 7
μb−1. The vm-vn correlations are measured in midrapidity
as a function of centrality, and, for events within the same
centrality interval, as a function of event ellipticity or
triangularity defined in a forward rapidity region. For
events within the same centrality interval, v3 is found to
be anticorrelated with v2 and this anticorrelation is
consistent with similar anticorrelations between the
corresponding eccentricities, ∊2 and ∊3. However, it is
observed that v4 increases strongly with v2, and v5
increases strongly with both v2 and v3. The trend and
strength of the vm-vn correlations for n = 4 and 5 are found
to disagree with ∊m-∊n correlations predicted by
initial-geometry models. Instead, these correlations are
found to be consistent with the combined effects of a linear
contribution to vn and a nonlinear term that is a function
of v22 or of v2v3, as predicted by hydrodynamic models. A
simple two-component fit is used to separate these two
contributions. The extracted linear and nonlinear
contributions to v4 and v5 are found to be consistent with
previously measured event-plane correlations.},
Doi = {10.1103/PhysRevC.92.034903},
Key = {fds313619}
}
@article{fds356785,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Measurement of the correlation between the polar angles of
leptons from top quark decays in the helicity basis at s =7
T e V using the ATLAS detector},
Journal = {Physical Review D},
Volume = {93},
Number = {1},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.93.012002},
Abstract = {A measurement of the correlations between the polar angles
of leptons from the decay of pair-produced t and t¯ quarks
in the helicity basis is reported, using proton-proton
collision data collected by the ATLAS detector at the LHC.
The dataset corresponds to an integrated luminosity of 4.6
fb-1 at a center-of-mass energy of s=7 TeV collected during
2011. Candidate events are selected in the dilepton topology
with large missing transverse momentum and at least two
jets. The angles θ1 and θ2 between the charged leptons and
the direction of motion of the parent quarks in the tt¯
rest frame are sensitive to the spin information, and the
distribution of cosθ1·cosθ2 is sensitive to the spin
correlation between the t and t¯ quarks. The distribution
is unfolded to parton level and compared to the
next-to-leading order prediction. A good agreement is
observed.},
Doi = {10.1103/PhysRevD.93.012002},
Key = {fds356785}
}
@article{fds374216,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames,
CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche,
CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Measurement of the CP properties of Higgs boson interactions
with τ -leptons with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11583-y},
Abstract = {A study of the charge conjugation and parity (CP) properties
of the interaction between the Higgs boson and τ -leptons
is presented. The study is based on a measurement of CP
-sensitive angular observables defined by the visible decay
products of τ -leptons produced in Higgs boson decays. The
analysis uses 139 fb- 1of proton–proton collision data
recorded at a centre-of-mass energy of s=13 TeV with the
ATLAS detector at the Large Hadron Collider. Contributions
from CP -violating interactions between the Higgs boson and
τ -leptons are described by a single mixing angle parameter
ϕτin the generalised Yukawa interaction. Without
constraining the H→ ττ signal strength to its expected
value under the Standard Model hypothesis, the mixing angle
ϕτis measured to be 9∘± 16∘, with an expected value
of 0∘± 28∘at the 68% confidence level. The pure CP -odd
hypothesis is disfavoured at a level of 3.4 standard
deviations. The results are compatible with the predictions
for the Higgs boson in the Standard Model.},
Doi = {10.1140/epjc/s10052-023-11583-y},
Key = {fds374216}
}
@article{fds307807,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Bousson, N and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
Title = {Measurement of the CP-violating phase βsJ/ψ in Bs0→J/ψ
decays with the CDF II detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.85.072002},
Abstract = {We present a measurement of the CP-violating parameter
βsJ/ψ using approximately 6500 Bs0→J/ψ decays
reconstructed with the CDF II detector in a sample of pp̄
collisions at √s=1.96TeV corresponding to 5.2fb -1
integrated luminosity produced by the Tevatron collider at
Fermilab. We find the CP-violating phase to be within the
range βsJ/ψ [0.02,0.52] [1.08,1.55] at 68% confidence
level where the coverage property of the quoted interval is
guaranteed using a frequentist statistical analysis. This
result is in agreement with the standard model expectation
at the level of about one Gaussian standard deviation. We
consider the inclusion of a potential S-wave contribution to
the Bs0→J/ψK +K - final state which is found to be
negligible over the mass interval 1.009<m(K +K
-)<1.028GeV/c2. Assuming the standard model prediction for
the CP-violating phase βsJ/ψ, we find the Bs0 decay width
difference to be ΔΓ s=0.075±0.035(stat) ±0.006(syst)ps
-1. We also present the most precise measurements of the Bs0
mean lifetime τ(Bs0)=1.529±0.025(stat) ±0.012(syst)ps,
the polarization fractions |A 0(0)|2=0. 524±0.013(stat)±0.015(syst)
and |A -(0)|2=0. 231±0.014(stat)±0.015(syst), as well as
the strong phase δ -=2.95±0.64(stat)±0.07(syst)rad. In
addition, we report an alternative Bayesian analysis that
gives results consistent with the frequentist approach. ©
2012 American Physical Society.},
Doi = {10.1103/PhysRevD.85.072002},
Key = {fds307807}
}
@article{fds356106,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
Title = {Measurement of the CP-violating phase ϕs in
Bs0→J/ψϕ decays in ATLAS at 13 TeV},
Journal = {European Physical Journal C},
Volume = {81},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09011-0},
Abstract = {A measurement of the Bs0→J/ψϕ decay parameters using
80.5fb-1 of integrated luminosity collected with the ATLAS
detector from 13 Te proton–proton collisions at the LHC
is presented. The measured parameters include the
CP-violating phase ϕs, the width difference Δ Γ s between
the Bs0 meson mass eigenstates and the average decay width
Γ s. The values measured for the physical parameters are
combined with those from 19.2fb-1 of 7 and 8 Te data,
leading to the following: ϕs=-0.087±0.036(stat.)±0.021(syst.)radΔΓs=0.0657±0.0043(stat.)±0.0037(syst.)ps-1Γs=0.6703±0.0014(stat.)±0.0018(syst.)ps-1Results
for ϕs and Δ Γ s are also presented as 68% confidence
level contours in the ϕs–Δ Γ s plane. Furthermore the
transversity amplitudes and corresponding strong phases are
measured. ϕs and Δ Γ s measurements are in agreement with
the Standard Model predictions.},
Doi = {10.1140/epjc/s10052-021-09011-0},
Key = {fds356106}
}
@article{fds321112,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of the CP-violating phase ϕsand the
Bs0meson decay width difference with
Bs0→ J/ψϕ decays in
ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)147},
Abstract = {A measurement of the Bs0decay parameters in the Bs0→
J/ψϕ channel using an integrated luminosity of 14.3
fb−1collected by the ATLAS detector from 8 TeV pp
collisions at the LHC is presented. The measured parameters
include the CP -violating phase ϕs, the decay width Γs and
the width difference between the mass eigenstates ΔΓs. The
values measured for the physical parameters are
statistically combined with those from 4.9 fb−1of 7 TeV
data, leading to the following: Φs = -0.090 ± 0.078
(stat.) ± (syst.) rad Δ Γs = 0.085 ± 0.011 (stat.) ±
0.007 (syst.) Ps-1 Δ Γs = 0.675 ± 0.003 (stat.) ± 0.03
(syst.) Ps-1 In the analysis the parameter ΔΓs is
constrained to be positive. Results for ϕs and ΔΓs are
also presented as 68% and 95% likelihood contours in the
ϕs-ΔΓs plane. Also measured in this decay channel are the
transversity amplitudes and corresponding strong phases. All
measurements are in agreement with the Standard Model
predictions.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP08(2016)147},
Key = {fds321112}
}
@article{fds307594,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and d'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucà, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the cross section for direct-photon
production in association with a heavy quark in pp[over ¯]
collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {111},
Number = {4},
Pages = {042003},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.111.042003},
Abstract = {We report on a measurement of the cross section for
direct-photon production in association with a heavy quark
using the full data set of sqrt[s]=1.96 TeV
proton-antiproton collisions corresponding to 9.1 fb-1
of integrated luminosity collected by the CDF II detector at
the Fermilab Tevatron. The measurements are performed as a
function of the photon transverse momentum, covering a
photon transverse momentum between 30 and 300 GeV, photon
rapidities |yγ|<1.0, a heavy-quark-jet transverse momentum
pTjet>20 GeV, and jet rapidities |yjet|<1.5. The
results are compared with several theoretical
predictions.},
Doi = {10.1103/physrevlett.111.042003},
Key = {fds307594}
}
@article{fds356747,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the cross section for inclusive
isolated-photon production in pp collisions at s=13 TeV
using the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {770},
Pages = {473-493},
Year = {2017},
Month = {July},
url = {http://dx.doi.org/10.1016/j.physletb.2017.04.072},
Abstract = {Inclusive isolated-photon production in pp collisions at a
centre-of-mass energy of 13 TeV is studied with the ATLAS
detector at the LHC using a data set with an integrated
luminosity of 3.2 fb−1. The cross section is measured as a
function of the photon transverse energy above 125 GeV in
different regions of photon pseudorapidity.
Next-to-leading-order perturbative QCD and Monte Carlo
event-generator predictions are compared to the
cross-section measurements and provide an adequate
description of the data.},
Doi = {10.1016/j.physletb.2017.04.072},
Key = {fds356747}
}
@article{fds356684,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the cross section for isolated-photon plus
jet production in ppcollisions at √s=13TeV using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {780},
Pages = {578-602},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2018.03.035},
Abstract = {The dynamics of isolated-photon production in association
with a jet in proton–proton collisions at a centre-of-mass
energy of 13 TeV are studied with the ATLAS detector at the
LHC using a dataset with an integrated luminosity of 3.2
fb−1. Photons are required to have transverse energies
above 125 GeV. Jets are identified using the anti-kt
algorithm with radius parameter R=0.4 and required to have
transverse momenta above 100 GeV. Measurements of
isolated-photon plus jet cross sections are presented as
functions of the leading-photon transverse energy, the
leading-jet transverse momentum, the azimuthal angular
separation between the photon and the jet, the photon–jet
invariant mass and the scattering angle in the photon–jet
centre-of-mass system. Tree-level plus parton-shower
predictions from SHERPA and PYTHIA as well as
next-to-leading-order QCD predictions from JETPHOX and
SHERPA are compared to the measurements.},
Doi = {10.1016/j.physletb.2018.03.035},
Key = {fds356684}
}
@article{fds308131,
Author = {Acosta, and D, and others},
Title = {Measurement of the cross section for prompt diphoton
production in p anti-p collisions at sqrt[s]=1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {95},
Number = {2},
Pages = {022003},
Year = {2005},
url = {http://dx.doi.org/10.1103/physrevlett.95.022003},
Abstract = {http://arxiv.org/abs/hep-ex/0412050},
Doi = {10.1103/physrevlett.95.022003},
Key = {fds308131}
}
@article{fds307838,
Author = {Aaltonen, TEA},
Title = {Measurement of the Cross Section for Prompt Isolated
Diphoton Production in $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {10},
Pages = {102003},
Publisher = {American Physical Society},
Year = {2011},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.102003},
Abstract = {This Letter reports a measurement of the cross section of
prompt isolated photon pair production in pp collisions at a
total energy square root(s)=1.96 TeV using data of
5.36 fb(-1) integrated luminosity collected with the
CDF II detector at the Fermilab Tevatron. The measured cross
section, differential in basic kinematic variables, is
compared with three perturbative QCD predictions, a leading
order parton shower calculation and two next-to-leading
order calculations. The next-to-leading order calculations
reproduce most aspects of the data. By including photon
radiation from quarks before and after hard scattering, the
parton shower prediction becomes competitive with the
next-to-leading order predictions.},
Doi = {10.1103/PhysRevLett.107.102003},
Key = {fds307838}
}
@article{fds307612,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov,
A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Riddick, T and Rimondi,
F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani,
M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu,
V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song,
H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the cross section for prompt isolated
diphoton production using the full CDF run II data
sample.},
Journal = {Physical review letters},
Volume = {110},
Number = {10},
Pages = {101801},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.110.101801},
Abstract = {This Letter reports a measurement of the cross section for
producing pairs of central prompt isolated photons in
proton-antiproton collisions at a total energy sqrt[s] =
1.96 TeV using data corresponding to 9.5 fb(-1) integrated
luminosity collected with the CDF II detector at the
Fermilab Tevatron. The measured differential cross section
is compared to three calculations derived from the theory of
strong interactions. These include a prediction based on a
leading order matrix element calculation merged with a
parton shower model, a next-to-leading order calculation,
and a next-to-next-to-leading order calculation. The first
and last calculations reproduce most aspects of the data,
thus showing the importance of higher-order contributions
for understanding the theory of strong interaction and
improving measurements of the Higgs boson and searches for
new phenomena in diphoton final states.},
Doi = {10.1103/physrevlett.110.101801},
Key = {fds307612}
}
@article{fds308153,
Author = {Acosta, and D, and others},
Title = {Measurement of the cross section for t anti-t production in
p anti-p collisions using the kinematics of lepton + jets
events},
Journal = {Phys. Rev.},
Volume = {D72},
Number = {5},
Pages = {052003},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.72.052003},
Abstract = {http://arxiv.org/abs/hep-ex/0504053},
Doi = {10.1103/PhysRevD.72.052003},
Key = {fds308153}
}
@article{fds307756,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the cross section for the production of a W
boson in association with b-jets in pp collisions at √s =
7 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {707},
Number = {5},
Pages = {418-437},
Publisher = {Elsevier BV},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2011.12.046},
Abstract = {A measurement is presented of the cross section for the
production of a W boson with one or two jets, of which at
least one must be a b-jet, in pp collisions at √s = 7 TeV.
Production via top decay is not included in the signal
definition. The measurement is based on 35 pb-1 of data
collected with the ATLAS detector at the LHC. The W + b-jet
cross section is defined for jets reconstructed with the
antikt clustering algorithm with transverse momentum above
25 GeV and rapidity within ±2.1. The b-jets are identified
by reconstructing secondary vertices. The fiducial cross
section is measured both for the electron and muon decay
channel of the W boson and is found to be 10.2 ± 1.9(stat)
± 2.6(syst) pb for one lepton flavour. The results are
compared with next-to-leading order QCD calculations, which
predict a cross section smaller than, though consistent
with, the measured value.},
Doi = {10.1016/j.physletb.2011.12.046},
Key = {fds307756}
}
@article{fds307733,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the cross section for top-quark pair
production in pp collisions at √s = 7 TeV with the ATLAS
detector using final states with two high-pT
leptons},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {5},
Publisher = {Springer Nature},
Year = {2012},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP05(2012)059},
Abstract = {A measurement is reported of the production cross section of
top-quark pairs (tt̄) in proton-proton collisions at a
center-of-mass energy of 7 TeV recorded with the ATLAS
detector at the LHC. Candidate events have a signature
consistent with containing two isolated leptons, large
missing transverse momentum, and at least two jets. Using a
data sample corresponding to an integrated luminosity of
0.70 fb-1, a tt̄ production cross section σtt̄ = 176 ±
5(stat.)-1111+(syst.) ± 8(lum.) pb is measured for an
assumed top-quark mass of mt = 172.5 GeV. This measurement
is in good agreement with Standard Model predictions. ©
CERN.},
Doi = {10.1007/JHEP05(2012)059},
Key = {fds307733}
}
@article{fds336988,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
Title = {Measurement of the cross section for W-boson production in
association with jets in pp̄ collisions at
s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {77},
Number = {1},
Year = {2008},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.77.011108},
Abstract = {We present a measurement of the cross section for W-boson
production in association with jets in pp̄ collisions at
s=1.96TeV. The analysis uses a data sample corresponding to
an integrated luminosity of 320pb-1 collected with the CDF
II detector. W bosons are identified in their electron decay
channel and jets are reconstructed using a cone algorithm.
For each W+≥n-jet sample (n=1-4) we measure the
differential cross section dσ(pp̄→W+≥
n-jet)/dETnth-jet×B(W→eν) with respect to the transverse
energy ET of the nth-highest ET jet above 20GeV, and the
total cross section σ(pp̄→W+≥n-jet;ETnth-jet>25GeV)×B(W→eν),
for a restricted W→eν decay phase space. The cross
sections, corrected for all detector effects, can be
directly compared to particle level W+jet(s) predictions. We
present here comparisons to leading order and
next-to-leading order predictions. © 2008 The American
Physical Society.},
Doi = {10.1103/PhysRevD.77.011108},
Key = {fds336988}
}
@article{fds317303,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of the cross section of high transverse momentum
Z→bb¯ production in proton–proton collisions at √s=8
TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {738},
Pages = {25-43},
Publisher = {Elsevier BV},
Year = {2014},
Month = {November},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2014.09.020},
Abstract = {This Letter reports the observation of a high transverse
momentum Z→bb¯ signal in proton–proton collisions at
s=8 TeV and the measurement of its production cross section.
The data analysed were collected in 2012 with the ATLAS
detector at the LHC and correspond to an integrated
luminosity of 19.5 fb−1. The Z→bb¯ decay is
reconstructed from a pair of b-tagged jets, clustered with
the anti-kt jet algorithm with R=0.4, that have low angular
separation and form a dijet with pT>200 GeV. The signal
yield is extracted from a fit to the dijet invariant mass
distribution, with the dominant, multi-jet background mass
shape estimated by employing a fully data-driven technique
that reduces the dependence of the analysis on simulation.
The fiducial cross section is determined to be
σZ→bb¯fid=2.02±0.20 (stat.) ±0.25 (syst.)±0.06
(lumi.) pb=2.02 ±0.33 pb, in good agreement with
next-to-leading-order theoretical predictions.},
Doi = {10.1016/j.physletb.2014.09.020},
Key = {fds317303}
}
@article{fds356579,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson,
TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Measurement of the cross-section and charge asymmetry of W
bosons produced in proton–proton collisions at √s=8TeV
with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {9},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7199-0},
Abstract = {This paper presents measurements of the W+→ μ+ν and
W-→ μ-ν cross-sections and the associated charge
asymmetry as a function of the absolute pseudorapidity of
the decay muon. The data were collected in proton–proton
collisions at a centre-of-mass energy of 8 TeV with the
ATLAS experiment at the LHC and correspond to a total
integrated luminosity of 20.2fb-1. The precision of the
cross-section measurements varies between 0.8 and 1.5% as a
function of the pseudorapidity, excluding the 1.9%
uncertainty on the integrated luminosity. The charge
asymmetry is measured with an uncertainty between 0.002 and
0.003. The results are compared with predictions based on
next-to-next-to-leading-order calculations with various
parton distribution functions and have the sensitivity to
discriminate between them.},
Doi = {10.1140/epjc/s10052-019-7199-0},
Key = {fds356579}
}
@article{fds307752,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the cross-section for b-jets produced in
association with a Z boson at s=7 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {706},
Number = {4-5},
Pages = {295-313},
Publisher = {Elsevier BV},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2011.11.059},
Abstract = {A measurement is presented of the inclusive cross-section
for b-jet production in association with a Z boson in pp
collisions at a centre-of-mass energy of s=7 TeV. The
analysis uses the data sample collected by the ATLAS
experiment in 2010, corresponding to an integrated
luminosity of approximately 36 pb-1. The event selection
requires a Z boson decaying into high pT electrons or muons,
and at least one b-jet, identified by its displaced vertex,
with transverse momentum pT>25 GeV and rapidity |y|<2.1.
After subtraction of background processes, the yield is
extracted from the vertex mass distribution of the candidate
b-jets. The ratio of this cross-section to the inclusive Z
cross-section (the average number of b-jets per Z event) is
also measured. Both results are found to be in good
agreement with perturbative QCD predictions at
next-to-leading order. © 2011 CERN.},
Doi = {10.1016/j.physletb.2011.11.059},
Key = {fds307752}
}
@article{fds356711,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the cross-section for electroweak production
of dijets in association with a Z boson in pp collisions at
s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {775},
Pages = {206-228},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2017.10.040},
Abstract = {The cross-section for the production of two jets in
association with a leptonically decaying Z boson (Zjj) is
measured in proton–proton collisions at a centre-of-mass
energy of 13 TeV, using data recorded with the ATLAS
detector at the Large Hadron Collider, corresponding to an
integrated luminosity of 3.2 fb−1. The electroweak Zjj
cross-section is extracted in a fiducial region chosen to
enhance the electroweak contribution relative to the
dominant Drell–Yan Zjj process, which is constrained using
a data-driven approach. The measured fiducial electroweak
cross-section is σEWZjj = 119±16(stat.)±20(syst.)±2(lumi.)
fb for dijet invariant mass greater than 250 GeV, and
34.2±5.8(stat.)±5.5(syst.)±0.7(lumi.) fb for dijet
invariant mass greater than 1 TeV. Standard Model
predictions are in agreement with the measurements. The
inclusive Zjj cross-section is also measured in six
different fiducial regions with varying contributions from
electroweak and Drell–Yan Zjj production.},
Doi = {10.1016/j.physletb.2017.10.040},
Key = {fds356711}
}
@article{fds356703,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Measurement of the cross-section for producing a W boson in
association with a single top quark in pp collisions at
√s=13 TeV with ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {1},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2018)063},
Abstract = {The inclusive cross-section for the associated production of
a W boson and top quark is measured using data from
proton-proton collisions at s=13 TeV. The dataset
corresponds to an integrated luminosity of 3.2 fb−1, and
was collected in 2015 by the ATLAS detector at the Large
Hadron Collider at CERN. Events are selected requiring two
opposite sign isolated leptons and at least one jet; they
are separated into signal and control regions based on their
jet multiplicity and the number of jets that are identified
as containing b hadrons. The W t signal is then separated
from the tt¯ background using boosted decision tree
discriminants in two regions. The cross-section is extracted
by fitting templates to the data distributions, and is
measured to be σW t = 94 ± 10(stat.)− 22+ 28(syst.) ±
2(lumi.) pb. The measured value is in good agreement with
the SM prediction of σtheory = 71.7±1.8 (scale)± 3.4
(PDF) pb [1].[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP01(2018)063},
Key = {fds356703}
}
@article{fds310343,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of the cross-section of high transverse momentum
vector bosons reconstructed as single jets and studies of
jet substructure in pp collisions at √s = 7 TeV with the
ATLAS detector},
Journal = {New Journal of Physics},
Volume = {16},
Number = {11},
Pages = {113013-113013},
Publisher = {IOP Publishing},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1088/1367-2630/16/11/113013},
Abstract = {This paper presents a measurement of the cross-section for
high transverse momentum W and Z bosons produced in pp
collisions and decaying to all-hadronic final states. The
data used in the analysis were recorded by the ATLAS
detector at the CERN Large Hadron Collider at a
centre-of-mass energy of and correspond to an integrated
luminosity of . The measurement is performed by
reconstructing the boosted W or Z bosons in single jets. The
reconstructed jet mass is used to identify the W and Z
bosons, and a jet substructure method based on energy
cluster information in the jet centre-of-mass frame is used
to suppress the large multi-jet background. The
cross-section for events with a hadronically decaying W or Z
boson, with transverse momentum and pseudorapidity , is
measured to be pb and is compared to next-to-leading-order
calculations. The selected events are further used to study
jet grooming techniques.},
Doi = {10.1088/1367-2630/16/11/113013},
Key = {fds310343}
}
@article{fds374210,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Measurement of the cross-sections of the electroweak and
total production of a Zγ pair in association with two jets
in pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {846},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138222},
Abstract = {This Letter presents the measurement of the fiducial and
differential cross-sections of the electroweak production of
a Zγ pair in association with two jets. The analysis uses
140 fb−1 of LHC proton–proton collision data taken at
s=13 TeV recorded by the ATLAS detector during the years
2015–2018. Events with a Z boson candidate decaying into
either an e+e− or μ+μ− pair, a photon and two jets are
selected. The electroweak component is extracted by
requiring a large dijet invariant mass and by using the
information about the centrality of the system and is
measured with an observed and expected significance well
above five standard deviations. The fiducial pp→Zγjj
cross-section for the electroweak production is measured to
be 3.6 ± 0.5 fb. The total fiducial cross-section that also
includes contributions where the jets arise from strong
interactions is measured to be 16.8−1.8+2.0 fb. The
results are consistent with the Standard Model predictions.
Differential cross-sections are also measured using the same
events and are compared with parton-shower Monte Carlo
simulations. Good agreement is observed between data and
predictions.},
Doi = {10.1016/j.physletb.2023.138222},
Key = {fds374210}
}
@article{fds356753,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Measurement of the D+ -meson production cross section at low
transverse momentum in pp¯ collisions at s=1.96
TeV},
Journal = {Physical Review D},
Volume = {95},
Number = {9},
Year = {2017},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.95.092006},
Abstract = {We report on a measurement of the D+-meson production cross
section as a function of transverse momentum (pT) in
proton-antiproton (pp) collisions at 1.96 TeV center-of-mass
energy, using the full data set collected by the Collider
Detector at Fermilab in Tevatron Run II and corresponding to
10 fb-1 of integrated luminosity. We use D+→K-π+π+
decays fully reconstructed in the central rapidity region
|y|<1 with transverse momentum down to 1.5 GeV/c, a range
previously unexplored in pp collisions. Inelastic
pp-scattering events are selected online using minimally
biasing requirements followed by an optimized offline
selection. The K-π+π+ mass distribution is used to
identify the D+ signal, and the D+ transverse
impact-parameter distribution is used to separate prompt
production, occurring directly in the hard-scattering
process, from secondary production from b-hadron decays. We
obtain a prompt D+ signal of 2950 candidates corresponding
to a total cross section σ(D+,1.5<pT<14.5
GeV/c,|y|<1)=71.9±6.8(stat)±9.3(syst) μb. While the
measured cross sections are consistent with theoretical
estimates in each pT bin, the shape of the observed pT
spectrum is softer than the expectation from quantum
chromodynamics. The results are unique in pp collisions and
can improve the shape and uncertainties of future
predictions.},
Doi = {10.1103/PhysRevD.95.092006},
Key = {fds356753}
}
@article{fds356771,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of the dependence of transverse energy
production at large pseudorapidity on the hard-scattering
kinematics of proton–proton collisions at √s=2.76 TeV
with ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {756},
Pages = {10-28},
Year = {2016},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2016.02.056},
Abstract = {The relationship between jet production in the central
region and the underlying-event activity in a
pseudorapidity-separated region is studied in 4.0 pb−1 of
s=2.76 TeV pp collision data recorded with the ATLAS
detector at the LHC. The underlying event is characterised
through measurements of the average value of the sum of the
transverse energy at large pseudorapidity downstream of one
of the protons, which are reported here as a function of
hard-scattering kinematic variables. The hard scattering is
characterised by the average transverse momentum and
pseudorapidity of the two highest transverse momentum jets
in the event. The dijet kinematics are used to estimate, on
an event-by-event basis, the scaled longitudinal momenta of
the hard-scattered partons in the target and projectile
beam-protons moving toward and away from the region
measuring transverse energy, respectively. Transverse energy
production at large pseudorapidity is observed to decrease
with a linear dependence on the longitudinal momentum
fraction in the target proton and to depend only weakly on
that in the projectile proton. The results are compared to
the predictions of various Monte Carlo event generators,
which qualitatively reproduce the trends observed in data
but generally underpredict the overall level of transverse
energy at forward pseudorapidity.},
Doi = {10.1016/j.physletb.2016.02.056},
Key = {fds356771}
}
@article{fds307812,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the difference in CP-violating asymmetries in
D(0)→K(+)K(-) and D(0)→π(+)π(-) decays at
CDF.},
Journal = {Physical review letters},
Volume = {109},
Number = {11},
Pages = {111801},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.109.111801},
Abstract = {We report a measurement of the difference (ΔA(CP)) between
time-integrated CP-violating asymmetries in D(0)→K(+)K(-)
and D(0)→π(+)π(-) decays reconstructed in the full data
set of proton-antiproton collisions collected by the
Collider Detector at Fermilab, corresponding to
9.7 fb(-1) of integrated luminosity. The strong decay
D(*+)→D(0)π(+) is used to identify the charm meson at
production as D(0) or D[over ¯](0). We measure
ΔA(CP)=[-0.62±0.21(stat)±0.10(syst)]%, which differs from
zero by 2.7 Gaussian standard deviations. This result
supports similar evidence for CP violation in charm-quark
decays obtained in proton-proton collisions.},
Doi = {10.1103/physrevlett.109.111801},
Key = {fds307812}
}
@article{fds307596,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Measurement of the differential cross section
dσ/d(cosθ(t)) for Top-Quark Pair Production in pp
Collisions at sqrt[s] = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {111},
Number = {18},
Pages = {182002},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.111.182002},
Abstract = {We report a measurement of the differential cross section
dσ/d(cosθ(t)) for top-quark pair production as a function
of the top-quark production angle in proton-antiproton
collisions at sqrt[s] = 1.96 TeV. This measurement is
performed using data collected with the CDF II detector at
the Tevatron, corresponding to an integrated luminosity of
9.4 fb(-1). We employ the Legendre polynomials to
characterize the shape of the differential cross section at
the parton level. The observed Legendre coefficients are in
good agreement with the prediction of the
next-to-leading-order standard-model calculation, with the
exception of an excess linear-term coefficient a(1) = 0.40
± 0.12, compared to the standard-model prediction of
a(1)=0.15(-0.03)(+0.07).},
Doi = {10.1103/physrevlett.111.182002},
Key = {fds307596}
}
@article{fds356635,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of the differential cross sections for W -boson
production in association with jets in p p collisions at s
=1.96 TeV MEASUREMENT of the DIFFERENTIAL CROSS ⋯ T.
AALTONEN et al.},
Journal = {Physical Review D},
Volume = {98},
Number = {11},
Year = {2018},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.98.112005},
Abstract = {This paper presents a study of the production of a single W
boson in association with one or more jets in
proton-antiproton collisions at s=1.96 TeV, using the entire
data set collected in 2001-2011 by the Collider Detector at
Fermilab at the Tevatron, which corresponds to an integrated
luminosity of 9.0 fb-1. The W boson is identified through
its leptonic decays into electron and muon. The production
cross sections are measured for each leptonic decay mode and
combined after testing that the ratio of the W(→μν)+jets
cross section to the W(→eν)+jets cross section agrees
with the hypothesis of e-μ lepton universality. The
combination of measured cross sections, differential in the
inclusive jet multiplicity (W+≥N jets with N=1, 2, 3, or
4) and in the transverse energy of the leading jet, are
compared with theoretical predictions.},
Doi = {10.1103/PhysRevD.98.112005},
Key = {fds356635}
}
@article{fds307570,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Measurement of the differential cross-section of B+ meson
production in pp collisions at √s = 7 TeV at
ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {10},
Pages = {1-37},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP10(2013)042},
Abstract = {The production cross-section of B+ mesons is measured as a
function of transverse momentum pT and rapidity y in
proton-proton collisions at centre-of-mass energy √s = 7
TeV, using 2.4 fb-1 of data recorded with the ATLAS detector
at the Large Hadron Collider. The differential production
cross-sections, determined in the range 9 GeV < pT < 120 GeV
and |y| < 2:25, are compared to next-to-leading-order
theoretical predictions. Copyright CERN.},
Doi = {10.1007/JHEP10(2013)042},
Key = {fds307570}
}
@article{fds356780,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Measurement of the differential cross-section of highly
boosted top quarks as a function of their transverse
momentum in s =8 TeV proton-proton collisions using the
ATLAS detector},
Journal = {Physical Review D},
Volume = {93},
Number = {3},
Year = {2016},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.93.032009},
Abstract = {The differential cross-section for pair production of top
quarks with high transverse momentum is measured in 20.3
fb-1 of proton-proton collisions at a center-of-mass energy
of 8 TeV. The measurement is performed for tt¯ events in
the lepton+jets channel. The cross-section is reported as a
function of the hadronically decaying top quark transverse
momentum for values above 300 GeV. The hadronically decaying
top quark is reconstructed as an anti-kt jet with radius
parameter R=1.0 and identified with jet substructure
techniques. The observed yield is corrected for detector
effects to obtain a cross-section at particle level in a
fiducial region close to the event selection. A parton-level
cross-section extrapolated to the full phase space is also
reported for top quarks with transverse momentum above 300
GeV. The predictions of a majority of next-to-leading-order
and leading-order matrix-element Monte Carlo generators are
found to agree with the measured cross-sections.},
Doi = {10.1103/PhysRevD.93.032009},
Key = {fds356780}
}
@article{fds323671,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {Measurement of the differential cross-sections of prompt and
non-prompt production of [Formula: see text] and [Formula:
see text] in pp collisions at [Formula: see text] and
8 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {283},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4050-8},
Abstract = {The production rates of prompt and non-prompt [Formula: see
text] and [Formula: see text] mesons in their dimuon decay
modes are measured using 2.1 and 11.4 fb[Formula: see text]
of data collected with the ATLAS experiment at the Large
Hadron Collider, in proton-proton collisions at [Formula:
see text] and 8 respectively. Production cross-sections for
prompt as well as non-prompt sources, ratios of [Formula:
see text] to [Formula: see text] production, and the
fractions of non-prompt production for [Formula: see text]
and [Formula: see text] are measured as a function of meson
transverse momentum and rapidity. The measurements are
compared to theoretical predictions.},
Doi = {10.1140/epjc/s10052-016-4050-8},
Key = {fds323671}
}
@article{fds308100,
Author = {Abulencia, and A, and others},
Title = {Measurement of the dipion mass spectrum in X(3872) --> J/psi
pi+ pi- decays},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {10},
Pages = {102002},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.102002},
Abstract = {We measure the dipion mass spectrum in X(3872) --> J/psi
pi++ pi+- decays using 360 pb-1 of p anti-p collisions at
s**(1/2) = 1.96 TeV collected with the CDF II detector. The
spectrum is fit with predictions for odd C-parity (3S_1,
1P_1, and 3D_J) charmonia decaying to J/psi pi++ pi+-, as
well as even C-parity states in which the pi+ons are from
rho0 decay. The latter case also encompasses exotic
interpretations, such as D0 D-bar*0 molecule. Only the 3S_1
and J/psi rho hypotheses are compatible with our data. Since
3S_1 is untenable on other grounds, decay via J/psi rho is
favored, which implies C = +1 for the X(3872). Models for
different J/psi-rho angular momenta L are considered.
Flexibility in the models, especially the introduction of
rho-omega interference, enable good descriptions of our data
for both L = 0 and 1.},
Doi = {10.1103/physrevlett.96.102002},
Key = {fds308100}
}
@article{fds307564,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Measurement of the distributions of event-by-event flow
harmonics in lead-lead collisions at √SNN =
2.76 TeV with the ATLAS detector at the LHC},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {11},
Publisher = {Springer Nature},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2013)183},
Abstract = {The distributions of event-by-event harmonic flow
coefficients υn for n = 2-4 are measured in √sNN =
2.76TeV Pb+Pb collisions using the ATLAS detector at the
LHC. The measurements are performed using charged particles
with transverse momentum pT > 0.5GeV and in the
pseudorapidity range |η| < 2.5 in a dataset of
approximately 7 μb-1 recorded in 2010. The shapes of the
υn distributions suggest that the associated flow vectors
are described by a two-dimensional Gaussian function in
central collisions for υ2 and over most of the measured
centrality range for υ3 and υ4. Significant deviations
from this function are observed for υ2 in mid-central and
peripheral collisions, and a small deviation is observed for
υ3 in mid-central collisions. In order to be sensitive to
these deviations, it is shown that the commonly used
multi-particle cumulants, involving four particles or more,
need to be measured with a precision better than a few
percent. The υn distributions are also measured
independently for charged particles with 0.5 < pT < 1 GeV
and pT > 1 GeV. When these distributions are rescaled to the
same mean values, the adjusted shapes are found to be nearly
the same for these two pT ranges. The υn distributions are
compared with the eccentricity distributions from two models
for the initial collision geometry: a Glauber model and a
model that includes corrections to the initial geometry due
to gluon saturation effects. Both models fail to describe
the experimental data consistently over most of the measured
centrality range. Copyright CERN.},
Doi = {10.1007/JHEP11(2013)183},
Key = {fds307564}
}
@article{fds321104,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Measurement of the double-differential high-mass Drell-Yan
cross section in pp collisions at √s = 8 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)009},
Abstract = {This paper presents a measurement of the double-differential
cross section for the Drell-Yan Z/γ∗ → ℓ+ℓ− and
photon-induced γγ → ℓ+ℓ− processes where ℓ is an
electron or muon. The measurement is performed for invariant
masses of the lepton pairs, mℓℓ, between 116 GeV and
1500 GeV using a sample of 20.3 fb−1 of pp collisions data
at centre-of-mass energy of s=8 TeV collected by the ATLAS
detector at the LHC in 2012. The data are presented double
differentially in invariant mass and absolute dilepton
rapidity as well as in invariant mass and absolute
pseudorapidity separation of the lepton pair. The
single-differential cross section as a function of mℓℓ
is also reported. The electron and muon channel measurements
are combined and a total experimental precision of better
than 1% is achieved at low mℓℓ. A comparison to
next-to-next-to-leading order perturbative QCD predictions
using several recent parton distribution functions and
including next-to-leading order electroweak effects
indicates the potential of the data to constrain parton
distribution functions. In particular, a large impact of the
data on the photon PDF is demonstrated.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP08(2016)009},
Key = {fds321104}
}
@article{fds356717,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurement of the Drell-Yan triple-differential cross
section in pp collisions at √s=8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {12},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2017)059},
Abstract = {This paper presents a measurement of the triple-differential
cross section for the Drell-Yan process Z/γ* → ℓ+ℓ−
where ℓ is an electron or a muon. The measurement is
performed for invariant masses of the lepton pairs, mℓℓ,
between 46 and 200 GeV using a sample of 20.2 fb−1 of pp
collisions data at a centre-of-mass energy of s=8 TeV
collected by the ATLAS detector at the LHC in 2012. The data
are presented in bins of invariant mass, absolute dilepton
rapidity, |yℓℓ|, and the angular variable cos θ*
between the outgoing lepton and the incoming quark in the
Collins-Soper frame. The measurements are performed in the
range |yℓℓ| < 2.4 in the muon channel, and extended to
|yℓℓ| < 3.6 in the electron channel. The cross sections
are used to determine the Z boson forward-backward asymmetry
as a function of |yℓℓ| and mℓℓ. The measurements
achieve high-precision, below the percent level in the pole
region, excluding the uncertainty in the integrated
luminosity, and are in agreement with predictions. These
precision data are sensitive to the parton distribution
functions and the effective weak mixing angle.},
Doi = {10.1007/JHEP12(2017)059},
Key = {fds356717}
}
@article{fds307545,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov,
VV and Dos Santos and SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
Title = {Measurement of the electroweak production of dijets in
association with a Z-boson and distributions sensitive to
vector boson fusion in proton-proton collisions at √s= 8
TeV using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {4},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP04(2014)031},
Doi = {10.1007/JHEP04(2014)031},
Key = {fds307545}
}
@article{fds363186,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari,
N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
Title = {Measurement of the energy asymmetry in tt¯ j production at
13 TeV with the ATLAS experiment and interpretation in the
SMEFT framework},
Journal = {European Physical Journal C},
Volume = {82},
Number = {4},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10101-w},
Abstract = {A measurement of the energy asymmetry in jet-associated
top-quark pair production is presented using 139fb-1 of data
collected by the ATLAS detector at the Large Hadron Collider
during pp collisions at s=13TeV. The observable measures the
different probability of top and antitop quarks to have the
higher energy as a function of the jet scattering angle with
respect to the beam axis. The energy asymmetry is measured
in the semileptonic tt¯ decay channel, and the hadronically
decaying top quark must have transverse momentum above
350GeV. The results are corrected for detector effects to
particle level in three bins of the scattering angle of the
associated jet. The measurement agrees with the SM
prediction at next-to-leading-order accuracy in quantum
chromodynamics in all three bins. In the bin with the
largest expected asymmetry, where the jet is emitted
perpendicular to the beam, the energy asymmetry is measured
to be - 0.043 ± 0.020 , in agreement with the SM prediction
of - 0.037 ± 0.003. Interpreting this result in the
framework of the Standard Model effective field theory
(SMEFT), it is shown that the energy asymmetry is sensitive
to the top-quark chirality in four-quark operators and is
therefore a valuable new observable in global SMEFT
fits.},
Doi = {10.1140/epjc/s10052-022-10101-w},
Key = {fds363186}
}
@article{fds362727,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Measurement of the energy response of the ATLAS calorimeter
to charged pions from W±→ τ±(→
π±ντ) ντ events in
Run 2 data},
Journal = {European Physical Journal C},
Volume = {82},
Number = {3},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10117-2},
Abstract = {The energy response of the ATLAS calorimeter is measured for
single charged pions with transverse momentum in the range
10 < pT< 300 GeV. The measurement is performed using 139 fb
- 1 of LHC proton–proton collision data at s=13 TeV taken
in Run 2 by the ATLAS detector. Charged pions originating
from τ-lepton decays are used to provide a sample of
high-pT isolated particles, where the composition is known,
to test an energy regime that has not previously been probed
by in situ single-particle measurements. The calorimeter
response to single-pions is observed to be overestimated by
∼ 2 % across a large part of the pT spectrum in the
central region and underestimated by ∼ 4 % in the endcaps
in the ATLAS simulation. The uncertainties in the
measurements are ≲ 1 % for 15 < pT< 185 GeV in the central
region. To investigate the source of the discrepancies, the
width of the distribution of the ratio of calorimeter energy
to track momentum, the energies per layer and response in
the hadronic calorimeter are also compared between data and
simulation.},
Doi = {10.1140/epjc/s10052-022-10117-2},
Key = {fds362727}
}
@article{fds356698,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the exclusive γγ → μ+μ−
process in proton–proton collisions at √s=13TeV with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {777},
Pages = {303-323},
Year = {2018},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2017.12.043},
Abstract = {The production of exclusive γγ→μ+μ− events in
proton–proton collisions at a centre-of-mass energy of 13
TeV is measured with the ATLAS detector at the LHC, using
data corresponding to an integrated luminosity of 3.2
fb−1. The measurement is performed for a dimuon invariant
mass of 12GeV<mμ+μ−<70GeV. The integrated cross-section
is determined within a fiducial acceptance region of the
ATLAS detector and differential cross-sections are measured
as a function of the dimuon invariant mass. The results are
compared to theoretical predictions both with and without
corrections for absorptive effects.},
Doi = {10.1016/j.physletb.2017.12.043},
Key = {fds356698}
}
@article{fds307631,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
M},
Title = {Measurement of the flavour composition of dijet events in pp
collisions at √s = 7 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {73},
Number = {2},
Publisher = {Springer Nature},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2301-5},
Abstract = {This paper describes a measurement of the flavour
composition of dijet events produced in pp collisions at
√s = 7 TeV using the ATLAS detector. The measurement uses
the full 2010 data sample, corresponding to an integrated
luminosity of 39 pb<sup>−1</sup>. Six possible
combinations of light, charm and bottom jets are identified
in the dijet events, where the jet flavour is defined by the
presence of bottom, charm or solely light flavour hadrons in
the jet. Kinematic variables, based on the properties of
displaced decay vertices and optimised for jet flavour
identification, are used in a multidimensional template fit
to measure the fractions of these dijet flavour states as
functions of the leading jet transverse momentum in the
range 40 GeV to 500 GeV and jet rapidity |y| < 2.1. The fit
results agree with the predictions of leading- and
next-to-leading-order calculations, with the exception of
the dijet fraction composed of bottom and light flavour
jets, which is underestimated by all models at large
transverse jet momenta. The ability to identify jets
containing two b-hadrons, originating from e.g. gluon
splitting, is demonstrated. The difference between bottom
jet production rates in leading and subleading jets is
consistent with the next-to-leading-order
predictions.},
Doi = {10.1140/epjc/s10052-013-2301-5},
Key = {fds307631}
}
@article{fds321120,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Measurement of the forward-backward asymmetry in low-mass
bottom-quark pairs produced in proton-antiproton
collisions},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112003},
Abstract = {We report a measurement of the forward-backward asymmetry,
AFB, in bb pairs produced in proton-antiproton collisions
and identified by muons from semileptonic b-hadron decays.
The event sample is collected at a center-of-mass energy of
s=1.96 TeV with the CDF II detector and corresponds to 6.9
fb-1 of integrated luminosity. We obtain an integrated
asymmetry of AFB(bb)=(1.2±0.7)% at the particle level for
b-quark pairs with invariant mass, mbb, down to 40 GeV/c2
and measure the dependence of AFB(bb) on mbb. The results
are compatible with expectations from the standard
model.},
Doi = {10.1103/PhysRevD.93.112003},
Key = {fds321120}
}
@article{fds307873,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the Forward-Backward Asymmetry in the
${B}\rightarrow{K}^{(*)}\mu^{+}\mu^{-}$ Decay and First
Observation of the ${B}_{s}^{0}$\rightarrow${}$\phi${}{$\mu${}}^{+}{$\mu${}}^{-}$
Decay},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {16},
Pages = {161801},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.161801},
Abstract = {We reconstruct the rare decays B(+)→K(+)μ(+0μ(-0,
B90)→K*(892)(0)μ(+)μ(-), and B(s)(0)→ϕ(1020)μ(+)μ(-)
in a data sample corresponding to 4.4 fb(-1) collected
in pp collisions at √[s]=1.96 TeV by the CDF II
detector at the Tevatron Collider. Using 121±16
B(+)→K(+)μ(+)μ(-) and 101±12 B(0)→K(*0)μ(+)μ(-)
decays we report the branching ratios. In addition, we
report the differential branching ratio and the muon
forward-backward asymmetry in the B(+) and B(0) decay modes,
and the K(*0) longitudinal polarization fraction in the B(0)
decay mode with respect to the squared dimuon mass. These
are consistent with the predictions, and most recent
determinations from other experiments and of comparable
accuracy. We also report the first observation of the
B(s)(0)→ϕμ(+)μ(-) decay and measure its branching ratio
BR(B(s)(0)→ϕμ(+)μ(-))=[1.44±0.33±0.46]×10(-6) using
27±6 signal events. This is currently the most rare B(s)(0)
decay observed.},
Doi = {10.1103/PhysRevLett.106.161801},
Key = {fds307873}
}
@article{fds313597,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the forward-backward asymmetry of electron
and muon pair-production in pp collisions at √s=7 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {9},
Pages = {1-43},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2015)049},
Abstract = {This paper presents measurements from the ATLAS experiment
of the forward-backward asymmetry in the reaction pp →
Z/γ* → l+l−, with l being electrons or muons, and the
extraction of the effective weak mixing angle. The results
are based on the full set of data collected in 2011 in pp
collisions at the LHC at (Formula presented.), corresponding
to an integrated luminosity of 4.8 fb−1. The measured
asymmetry values are found to be in agreement with the
corresponding Standard Model predictions. The combination of
the muon and electron channels yields a value of the
effective weak mixing angle of sin2θefflept = 0.2308 ±
0.0005(stat.) ± 0.0006(syst.) ± 0.0009(PDF), where the
first uncertainty corresponds to data statistics, the second
to systematic effects and the third to knowledge of the
parton density functions. This result agrees with the
current world average from the Particle Data Group
fit.},
Doi = {10.1007/JHEP09(2015)049},
Key = {fds313597}
}
@article{fds321121,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Measurement of the forward-backward asymmetry of top-quark
and antiquark pairs using the full CDF Run II data
set},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112005},
Abstract = {We measure the forward-backward asymmetry of the production
of top-quark and antiquark pairs in proton-antiproton
collisions at center-of-mass energy s=1.96 TeV using the
full data set collected by the Collider Detector at Fermilab
(CDF) in Tevatron Run II corresponding to an integrated
luminosity of 9.1 fb-1. The asymmetry is characterized by
the rapidity difference between top quarks and antiquarks
(Δy) and measured in the final state with two charged
leptons (electrons and muons). The inclusive asymmetry,
corrected to the entire phase space at parton level, is
measured to be AFBtt=0.12±0.13, consistent with the
expectations from the standard model (SM) and previous CDF
results in the final state with a single charged lepton. The
combination of the CDF measurements of the inclusive AFBtt
in both final states yields AFBtt=0.160±0.045, which is
consistent with the SM predictions. We also measure the
differential asymmetry as a function of Δy. A linear fit to
AFBtt(|Δy|), assuming zero asymmetry at Δy=0, yields a
slope of α=0.14±0.15, consistent with the SM prediction
and the previous CDF determination in the final state with a
single charged lepton. The combined slope of AFBtt(|Δy|) in
the two final states is α=0.227±0.057, which is 2.0σ
larger than the SM prediction.},
Doi = {10.1103/PhysRevD.93.112005},
Key = {fds321121}
}
@article{fds323244,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen,
D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy,
L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard,
PF},
Title = {Measurement of the forward-backward charge asymmetry from
W→ev production in pp̄ collisions at √s=1.96
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {5},
Pages = {1-9},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.051104},
Abstract = {We report a measurement of the forward-backward charge
asymmetry of electrons from W boson decays in pp̄
collisions at √s=1.96 TeV using a data sample of 170 pb-1
collected by the Collider Detector at Fermilab. The
asymmetry is measured as a function of electron rapidity and
transverse energy and provides new input on the momentum
fraction dependence of the u and d quark parton distribution
functions within the proton. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevD.71.051104},
Key = {fds323244}
}
@article{fds356612,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S},
Title = {Measurement of the four-lepton invariant mass spectrum in 13
TeV proton-proton collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {4},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2019)048},
Abstract = {A measurement of the four-lepton invariant mass spectrum is
made with the ATLAS detector, using an integrated luminosity
of 36.1 fb−1 of proton-proton collisions at s = 13 TeV
delivered by the Large Hadron Collider. The differential
cross-section is measured for events containing two
same-flavour opposite-sign lepton pairs. It exhibits a rich
structure, with different mass regions dominated in the
Standard Model by single Z boson production, Higgs boson
production, and Z boson pair production, and non-negligible
interference effects at high invariant masses. The
measurement is compared with state-of-the-art Standard Model
calculations, which are found to be consistent with the
data. These calculations are used to interpret the data in
terms of gg → ZZ → 4ℓ and Z → 4ℓ subprocesses, and
to place constraints on a possible contribution from physics
beyond the Standard Model.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP04(2019)048},
Key = {fds356612}
}
@article{fds337969,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Copic, K and Cordelli, M and Cortiana, G and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson,
R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and Barbaro,
PD and Cecco, SD and Deisher, A and Lorenzo, GD and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler,
A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes,
RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori,
M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, SW and Leone, S and Lewis, JD and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, RS and Lucchesi, D and Lueck,
J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou,
A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pinera, L and Pitts,
K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn,
F and Pronko, A and Proudfoot, J and Ptohos, F and Pueschel, E and Punzi,
G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle,
T and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shiraishi,
S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith,
JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B},
Title = {Measurement of the fraction of tt̄ production via
gluon-gluon fusion in pp̄ collisions at
s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {3},
Pages = {031101},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.031101},
Abstract = {We present a measurement of the ratio of the tt̄ production
cross section via gluon-gluon fusion to the total tt̄
production cross section in pp̄ collisions at s=1.96TeV at
the Tevatron. Using a data sample with an integrated
luminosity of 955pb-1 recorded by the CDF II detector at
Fermilab, we select events based on the tt̄ decay to
lepton+jets. Using an artificial neural network technique we
discriminate between tt̄ events produced via qq̄
annihilation and gg fusion, and find Gf=σ(gg→tt̄)/
σ(pp̄→tt̄)<0.33 at the 68% confidence level. This
result is combined with a previous measurement to obtain the
most stringent measurement of this quantity by CDF to date,
Gf=0.07-0.07+0.15. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.031101},
Key = {fds337969}
}
@article{fds308077,
Author = {Abulencia, and A, and others},
Title = {Measurement of the Helicity Fractions of W Bosons from Top
Quark Decays using Fully Reconstructed \boldmath${t\bar{t}}$
Events with CDF II},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {5},
Pages = {052001},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.052001},
Abstract = {We present a measurement of the fractions F0 and F+ of
longitudinally polarized and right-handed W bosons in
top-quark decays using data collected with the CDF II
detector. The data set used in the analysis corresponds to
an integrated luminosity of approximately 318 pb-1. We
select t[overline t] candidate events with one lepton, at
least four jets, and missing transverse energy. Our helicity
measurement uses the decay angle theta*, which is defined as
the angle between the momentum of the charged lepton in the
W boson rest frame and the W momentum in the top-quark rest
frame. The costheta* distribution in the data is determined
by full kinematic reconstruction of the t[overline t]
candidates. We find F0=0.85-0.22+0.15(stat)$\pm$0.06(syst)
and F+=0.05-0.05+0.11(stat)$\pm$0.03(syst), which is
consistent with the standard model prediction. We set an
upper limit on the fraction of right-handed W bosons of
F+},
Doi = {10.1103/PhysRevD.75.052001},
Key = {fds308077}
}
@article{fds308111,
Author = {collaboration, CDF},
Title = {Measurement of the Helicity of W Bosons in Top Quark
Decays},
Journal = {Phys.Rev.Lett.},
Volume = {84},
Number = {11},
Pages = {216-221},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.73.111103},
Abstract = {http://arXiv.org/ps/hep-ex/9909042},
Doi = {10.1103/PhysRevD.73.111103},
Key = {fds308111}
}
@article{fds356693,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the Higgs boson coupling properties in the H
→ ZZ ∗ → 4ℓ decay channel at √s=13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {3},
Year = {2018},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2018)095},
Abstract = {The coupling properties of the Higgs boson are studied in
the four-lepton (e, μ) decay channel using 36.1 fb−1 of
pp collision data from the LHC at a centre-of-mass energy of
13 TeV collected by the ATLAS detector. Cross sections are
measured for the main production modes in several exclusive
regions of the Higgs boson production phase space and are
interpreted in terms of coupling modifiers. The inclusive
cross section times branching ratio for H → ZZ∗ decay
and for a Higgs boson absolute rapidity below 2.5 is
measured to be 1. 73− 0.23+ 0.24(stat.)− 0.08+
0.10(exp.) ± 0.04(th.) pb compared to the Standard Model
prediction of 1.34±0.09 pb. In addition, the tensor
structure of the Higgs boson couplings is studied using an
effective Lagrangian approach for the description of
interactions beyond the Standard Model. Constraints are
placed on the non-Standard-Model CP-even and CP-odd
couplings to Z bosons and on the CP-odd coupling to
gluons.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP03(2018)095},
Key = {fds356693}
}
@article{fds310360,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abidi, SH and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the Higgs boson mass from the H → γγ and
H → ZZ∗- 4ℓ channels inpp collisions at
center-of-mass energies of 7 and 8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052004},
Abstract = {An improved measurement of the mass of the Higgs boson is
derived from a combined fit to the reconstructed invariant
mass spectra of the decay channels H → γγ and H →
ZZ∗→ 4ℓ. The analysis uses the pp collision data
sample recorded by the ATLAS experiment at the CERN Large
Hadron Collider at center-of-mass energies of 7 TeV and 8
TeV, corresponding to an integrated luminosity of 25 fb-1.
The measured value of the Higgs boson mass is mH= 125.36 ±
0.37(stat) ± 0.18(syst) GeV. This result is based on
improved energy-scale calibrations for photons, electrons,
and muons as well as other analysis improvements, and
supersedes the previous result from ATLAS. Upper limits on
the total width of the Higgs boson are derived from fits to
the invariant mass spectra of the H → γγ and H →
ZZ∗→ 4ℓ decay channels.},
Doi = {10.1103/PhysRevD.90.052004},
Key = {fds310360}
}
@article{fds356662,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Measurement of the Higgs boson mass in the
H → ZZ⁎ → 4ℓ and H → γγ
channels with s=13 TeV pp collisions using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {784},
Pages = {345-366},
Year = {2018},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2018.07.050},
Abstract = {The mass of the Higgs boson is measured in the
H→ZZ⁎→4ℓ and in the H→γγ decay channels with
36.1 fb−1 of proton–proton collision data from the Large
Hadron Collider at a centre-of-mass energy of 13 TeV
recorded by the ATLAS detector in 2015 and 2016. The
measured value in the H→ZZ⁎→4ℓ channel is
mHZZ⁎=124.79±0.37GeV, while the measured value in the
H→γγ channel is mHγγ=124.93±0.40GeV. Combining these
results with the ATLAS measurement based on 7 and 8 TeV
proton–proton collision data yields a Higgs boson mass of
mH=124.97±0.24GeV.},
Doi = {10.1016/j.physletb.2018.07.050},
Key = {fds356662}
}
@article{fds372123,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V},
Title = {Measurement of the Higgs boson mass in the
H → ZZ⁎ → 4ℓ decay channel using
139 fb−1 of s=13 TeV pp collisions recorded by
the ATLAS detector at the LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137880},
Abstract = {The mass of the Higgs boson is measured in the
H→ZZ⁎→4ℓ decay channel. The analysis uses
proton–proton collision data from the Large Hadron
Collider at a centre-of-mass energy of 13 TeV recorded by
the ATLAS detector between 2015 and 2018, corresponding to
an integrated luminosity of 139 fb−1. The measured value
of the Higgs boson mass is 124.99±0.18(stat.)±0.04(syst.)
GeV. In final states with muons, this measurement benefits
from an improved momentum-scale calibration relative to that
adopted in previous publications. The measurement also
employs an analytic model that takes into account the
invariant-mass resolution of the four-lepton system on a
per-event basis and the output of a deep neural network
discriminating signal from background events. This
measurement is combined with the corresponding measurement
using 7 and 8 TeV pp collision data, resulting in a Higgs
boson mass of 124.94±0.17(stat.)±0.03(syst.)
GeV.},
Doi = {10.1016/j.physletb.2023.137880},
Key = {fds372123}
}
@article{fds375875,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Measurement of the Higgs boson mass with H → γγ
decays in 140 fb−1 of s=13 TeV pp collisions
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {847},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138315},
Abstract = {The mass of the Higgs boson is measured in the H→γγ
decay channel, exploiting the high resolution of the
invariant mass of photon pairs reconstructed from the decays
of Higgs bosons produced in proton–proton collisions at a
centre-of-mass energy s=13 TeV. The dataset was collected
between 2015 and 2018 by the ATLAS detector at the Large
Hadron Collider, and corresponds to an integrated luminosity
of 140 fb−1. The measured value of the Higgs boson mass is
125.17±0.11(stat.)±0.09(syst.) GeV and is based on an
improved energy scale calibration for photons, whose impact
on the measurement is about four times smaller than in the
previous publication. A combination with the corresponding
measurement using 7 and 8 TeV pp collision ATLAS data
results in a Higgs boson mass measurement of
125.22±0.11(stat.)±0.09(syst.) GeV. With an uncertainty of
1.1 per mille, this is currently the most precise
measurement of the mass of the Higgs boson from a single
decay channel.},
Doi = {10.1016/j.physletb.2023.138315},
Key = {fds375875}
}
@article{fds308216,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E},
Title = {Measurement of the high-mass drell-yan cross section and
limits on quark-electron compositeness scales},
Journal = {Physical Review Letters},
Volume = {82},
Number = {24},
Pages = {4769-4774},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.4769},
Abstract = {We present a measurement of the Drell-Yan cross section at
high dielectron invariant mass using 120 pb-1 of data
collected in pp collisions at √ s = 1.8 TeV by the D0
Collaboration during 1992-1996. No deviation from standard
model expectations is observed. We use the data to set
limits on the quark-electron compositeness scale. The 95%
confidence level lower limits on the compositeness scale
vary between 3.3 and 6.1 TeV depending on the assumed form
of the effective contact interaction. © 1999 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.82.4769},
Key = {fds308216}
}
@article{fds307647,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Measurement of the high-mass Drell–Yan differential
cross-section in pp collisions at √s=7TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {725},
Number = {4-5},
Pages = {223-242},
Publisher = {Elsevier BV},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2013.07.049},
Abstract = {This Letter reports a measurement of the high-mass
Drell–Yan differential cross-section in proton–proton
collisions at a centre-of-mass energy of 7 TeV at the LHC.
Based on an integrated luminosity of 4.9 fb−1, the
differential cross-section in the Z/γ⁎→e+e− channel
is measured with the ATLAS detector as a function of the
invariant mass, mee, in the range 116 <mee <1500 GeV, for a
fiducial region in which both the electron and the positron
have transverse momentum pT >25 GeV and pseudorapidity |η|
<2.5. A comparison is made to various event generators and
to the predictions of perturbative QCD calculations at
next-to-next-to-leading order.},
Doi = {10.1016/j.physletb.2013.07.049},
Key = {fds307647}
}
@article{fds375363,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
S and Ai, X and Aielli, G and Aikot, A and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Dos Santos,
SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA},
Title = {Measurement of the H→ γγ and H→ ZZ∗→ 4
ℓ cross-sections in pp collisions at √s=13.6 TeV with
the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {84},
Number = {1},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-12130-5},
Abstract = {The inclusive Higgs boson production cross-section is
measured in the di-photon and the ZZ∗→ 4 ℓ decay
channels using 31.4 and 29.0 fb - 1 of pp collision data
respectively, collected with the ATLAS detector at a
centre-of-mass energy of s=13.6 TeV . To reduce the model
dependence, the measurement in each channel is restricted to
a particle-level phase space that closely matches the
channel’s detector-level kinematic selection, and it is
corrected for detector effects. These measured fiducial
cross-sections are σfid,γγ= 76-13+14 fb, and σfid,4ℓ=
2.80±0.74 fb, in agreement with the corresponding Standard
Model predictions of 67.6 ± 3.7 fb and 3.67 ± 0.19 fb.
Assuming Standard Model acceptances and branching fractions
for the two channels, the fiducial measurements are
extrapolated to the full phase space yielding total
cross-sections of σ(pp→H)=67-11+12 pb and 46 ± 12 pb at
13.6 TeV from the di-photon and ZZ∗→ 4 ℓ measurements
respectively. The two measurements are combined into a total
cross-section measurement of σ(pp→ H) = 58.2 ± 8.7 pb,
to be compared with the Standard Model prediction of
σ(pp→ H) SM= 59.9 ± 2.6 pb.},
Doi = {10.1140/epjc/s10052-023-12130-5},
Key = {fds375363}
}
@article{fds325309,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, A and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoros, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antosb, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchou, C and Bendel, M and Benekos,
N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Boeser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
G and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Buescher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
JM and Buttinger, W and Byatt, T and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito,
L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman, JD and Chapman,
JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
Title = {Measurement of the inclusive and dijet cross-sections of
b-jets in pp collisions at √s=7 TeV
with the ATLAS detector},
Journal = {EUROPEAN PHYSICAL JOURNAL C},
Volume = {71},
Number = {12},
Publisher = {Springer New York LLC},
Year = {2011},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1846-4},
Abstract = {The inclusive and dijet production cross-sections have been
measured for jets containing b-hadrons (b-jets) in
proton-proton collisions at a centre-of-mass energy of +fs =
7 TeV, using the ATLAS detector at the LHC. The measurements
use data corresponding to an integrated luminosity of 34
pb_1. The b-jets are identified using either a
lifetime-based method, where secondary decay vertices of
b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the
presence of a muon is used to identify semileptonic decays
of b-hadrons inside jets. The inclusive b-jet cross-section
is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range \y\ < 2.1.
The bb-dijet cross-section is measured as a function of the
dijet invariant mass in the range 110 < mjj < 760 GeV, the
azimuthal angle difference between the two jets and the
angular variable χ in two dijet mass regions. The results
are compared with next-to-leading-order QCD predictions.
Good agreement is observed between the measured
cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the
measured bb-dijet cross-section. However, it does not
reproduce the measured inclusive cross-section well,
particularly for central b-jets with large transverse
momenta.},
Doi = {10.1140/epjc/s10052-011-1846-4},
Key = {fds325309}
}
@article{fds347477,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
Title = {Measurement of the inclusive and fiducial t t ¯ production
cross-sections in the lepton+jets channel in pp
collisions at s = 8 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {6},
Pages = {487},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5904-z},
Abstract = {The inclusive and fiducial t t ¯ production cross-sections
are measured in the lepton+jets channel using 20.2 fb - 1 of
proton-proton collision data at a centre-of-mass energy of 8
TeV recorded with the ATLAS detector at the LHC. Major
systematic uncertainties due to the modelling of the jet
energy scale and <i>b</i>-tagging efficiency are constrained
by separating selected events into three disjoint regions.
In order to reduce systematic uncertainties in the most
important background, the W +\,jets process is modelled
using Z + jets events in a data-driven approach. The
inclusive t t ¯ cross-section is measured with a precision
of 5.7% to be σ inc ( t t ¯ ) = 248.3 ± 0.7 ( stat . ) ±
13.4 ( syst . ) ± 4.7 ( lumi . ) pb , assuming a top-quark
mass of 172.5 GeV. The result is in agreement with the
Standard Model prediction. The cross-section is also
measured in a phase space close to that of the selected
data. The fiducial cross-section is σ fid ( t t ¯ ) = 48.8
± 0.1 ( stat . ) ± 2.0 ( syst . ) ± 0.9 ( lumi . ) pb
with a precision of 4.5%.},
Doi = {10.1140/epjc/s10052-018-5904-z},
Key = {fds347477}
}
@article{fds356566,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Measurement of the inclusive cross-section for the
production of jets in association with a Z boson in
proton–proton collisions at 8 TeV using the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {10},
Year = {2019},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7321-3},
Abstract = {The inclusive cross-section for jet production in
association with a Z boson decaying into an
electron–positron pair is measured as a function of the
transverse momentum and the absolute rapidity of jets using
19.9 fb- 1 of s=8 TeV proton–proton collision data
collected with the ATLAS detector at the Large Hadron
Collider. The measured Z+ jets cross-section is unfolded to
the particle level. The cross-section is compared with
state-of-the-art Standard Model calculations, including the
next-to-leading-order and next-to-next-to-leading-order
perturbative QCD calculations, corrected for
non-perturbative and QED radiation effects. The results of
the measurements cover final-state jets with transverse
momenta up to 1 TeV, and show good agreement with
fixed-order calculations.},
Doi = {10.1140/epjc/s10052-019-7321-3},
Key = {fds356566}
}
@article{fds356754,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Armitage, LJ and Arnaez, O},
Title = {Measurement of the inclusive cross-sections of single
top-quark and top-antiquark t-channel production in pp
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {4},
Year = {2017},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2017)086},
Abstract = {A measurement of the t-channel single-top-quark and
single-top-antiquark production cross-sections in the
lepton+jets channel is presented, using 3.2 fb−1 of
proton-proton collision data at a centre-of-mass energy of
13 TeV, recorded with the ATLAS detector at the LHC in 2015.
Events are selected by requiring one charged lepton
(electron or muon), missing transverse momentum, and two
jets with high transverse momentum, exactly one of which is
required to be b-tagged. Using a binned maximum-likelihood
fit to the discriminant distribution of a neural network,
the cross-sections are determined to be σ(tq) = 156 ± 5
(stat.) ± 27 (syst.) ± 3 (lumi.) pb for single top-quark
production and σ(t¯ q) = 91 ± 4 (stat.) ± 18 (syst.) ±
2 (lumi.) pb for single top-antiquark production, assuming a
top-quark mass of 172.5 GeV. The cross-section ratio is
measured to be Rt=σ(tq)/σ(t¯q)=1.72±0.09 (stat.) ± 0.18
(syst.). All results are in agreement with Standard Model
predictions.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP04(2017)086},
Key = {fds356754}
}
@article{fds308196,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk,
HE and Fisyak, Y and Flattum, E},
Title = {Measurement of the inclusive differential cross section for
Z bosons as a function of transverse momentum in [formula
presented] collisions at [formula presented]
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {61},
Number = {3},
Pages = {1-19},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.61.032004},
Abstract = {We present a measurement of the differential cross section
as a function of transverse momentum of the Z boson in
(Formula presented) collisions at (Formula presented) TeV
using data collected by the DØ experiment at the Fermilab
Tevatron Collider during 1994–1996. We find good agreement
between our data and the next-to-next-to-next-leading-logarithmic
resummation prediction and extract values of the
non-perturbative parameters for the resummed prediction from
a fit to the differential cross section. © 2000 The
American Physical Society.},
Doi = {10.1103/PhysRevD.61.032004},
Key = {fds308196}
}
@article{fds373463,
Author = {Jackson, P and Oliver, JL and Petridis, A and Qureshi, A and Sharma, AS and White, MJ and Cairo, VMM and Jain, V and Swift, SP and Gingrich, DM and Pinfold, JL and Sun, X and Wang, H and Cakir, O and Yildiz, HD and Kuday,
S and Turk Cakir and I and Sultansoy, S and Berger, N and Costanza, F and Dartsi, O and Delmastro, M and Di Ciaccio and L and Falke, PJ and Falke, S and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Kivernyk, O and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo
Martinez, N and Raspopov, S and Sauvan, E and Smart, BH and Todorova-Nova, S and Vallier, A and Wingerter-Seez, I and Abulaiti,
Y and Benjamin, DP and Chekanov, S and Hopkins, WH and LeCompte, T and Liu,
BX and Love, J and Malon, D and Metcalfe, J and Paramonov, A and Proudfoot,
J and Ryu, S and Stanek, RW and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Jones, S and Lampl, W and LeBlanc, M and Leone, R and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and De, K and Farbin, A and Griffiths, J and Hadavand, HK and Heelan, L and Little,
JD and Ozturk, N and Usai, G and White, A and Bellos, P and Fassouliotis,
D and Gkialas, I and Kourkoumelis, C and Papageorgiou, K and Tsirintanis, N and Alexopoulos, T and Bakalis, C and Benekos, N and Gazis, EN and Gkountoumis, P and Koulouris, A and Maltezos, S and Moschovakos, P and Panagoulias, I and Zacharis, G and Andeen, T and Narayan, R and Nikiforou, N and Onyisi, PUE and Potti,
H},
Title = {Measurement of the inclusive Formula Presented production
cross section in the lepton+jets channel in pp collisions at
Formula Presented with the ATLAS detector using support
vector machines},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032014},
Abstract = {A measurement of the top quark pair-production cross section
in the lepton + jets decay channel is presented. It is based
on 4.6 fb - 1 of s = 7 TeV p p collision data collected
during 2011 by the ATLAS experiment at the CERN Large Hadron
Collider. A three-class, multidimensional event classifier
based on support vector machines is used to differentiate t
t ¯ events from backgrounds. The t t ¯ production cross
section is found to be σ t t ¯ = 168.5 ± 0.7 ( stat ) -
5.9 + 6.2 ( syst ) - 3.2 + 3.4 ( lumi ) pb . The result is
consistent with the Standard Model prediction based on QCD
calculations at next-to-next-to-leading order.},
Doi = {10.1103/PhysRevD.108.032014},
Key = {fds373463}
}
@article{fds307999,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the inclusive isolated prompt photon cross
section in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
collisions at $\sqrt{s}=1.96\,\,TeV$ using the CDF
detector},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {11},
Pages = {111106},
Publisher = {American Physical Society},
Year = {2009},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.80.111106},
Abstract = {A measurement of the cross section for the inclusive
production of isolated photons by the CDF experiment at the
Fermilab Tevatron collider is presented. The measurement
covers the pseudorapidity region $|\eta\gamma|30$ GeV
and is based on 2.5 fb-1 of integrated luminosity. The
sample is almost a factor of 7 larger than those used for
recent published results and extends the $E_T^\gamma$
coverage by 100 GeV. The result agrees with next-to-leading
order perturbative QCD calculations within uncertainties
over the range $50},
Doi = {10.1103/PhysRevD.80.111106},
Key = {fds307999}
}
@article{fds321105,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold,
H},
Title = {Measurement of the inclusive isolated prompt photon cross
section in pp collisions at s=8TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)005},
Abstract = {Abstract: A measurement of the cross section for the
inclusive production of isolated prompt photons in
proton-proton collisions at a centre-of-mass energy of s=8
TeV is presented. The measurement covers the pseudorapidity
ranges |ηγ | < 1.37 and 1.56 ≤ |ηγ | < 2.37 in the
transverse energy range 25 < ETγ < 1500 GeV. The results
are based on an integrated luminosity of 20.2 fb−1,
recorded by the ATLAS detector at the LHC. Photon candidates
are identified by combining information from the
calorimeters and the inner tracker. The background is
subtracted using a data-driven technique, based on the
observed calorimeter shower-shape variables and the
deposition of hadronic energy in a narrow cone around the
photon candidate. The measured cross sections are compared
with leading-order and next-to-leading order perturbative
QCD calculations and are found to be in a good agreement
over ten orders of magnitude.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP08(2016)005},
Key = {fds321105}
}
@article{fds307857,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the inclusive isolated prompt photon
cross-section in pp collisions at √s=7 TeV using 35
pb-1 of ATLAS data},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {706},
Number = {2-3},
Pages = {150-167},
Publisher = {Elsevier BV},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2011.11.010},
Abstract = {A measurement of the differential cross-section for the
inclusive production of isolated prompt photons in pp
collisions at a center-of-mass energy √s=7 TeV is
presented. The measurement covers the pseudorapidity ranges
|η|<1.37 and 1.52≤|η|<2.37 in the transverse energy
range 45≤ET<400 GeV. The results are based on an
integrated luminosity of 35 pb-1, collected with the ATLAS
detector at the LHC. The yields of the signal photons are
measured using a data-driven technique, based on the
observed distribution of the hadronic energy in a narrow
cone around the photon candidate and the photon selection
criteria. The results are compared with next-to-leading
order perturbative QCD calculations and found to be in good
agreement over four orders of magnitude in cross-section. ©
2011 CERN.},
Doi = {10.1016/j.physletb.2011.11.010},
Key = {fds307857}
}
@article{fds307548,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Measurement of the inclusive isolated prompt photons cross
section in pp collisions at √s =7 TeV with the ATLAS
detector using 4.6 fb-1},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.89.052004},
Abstract = {A measurement of the cross section for the production of
isolated prompt photons in pp collisions at a center-of-mass
energy √s=7 TeV is presented. The results are based on an
integrated luminosity of 4.6 fb-1 collected with the ATLAS
detector at the LHC. The cross section is measured as a
function of photon pseudorapidity ηγ and transverse energy
ETγ in the kinematic range 100≤ETγ<1000 GeV and in the
regions |ηγ|<1.37 and 1.52≤|ηγ|<2.37. The results are
compared to leading-order parton-shower Monte Carlo models
and next-to-leading-order perturbative QCD calculations.
Next-to-leading-order perturbative QCD calculations agree
well with the measured cross sections as a function of ETγ
and ηγ.},
Doi = {10.1103/PhysRevD.89.052004},
Key = {fds307548}
}
@article{fds356569,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Measurement of the inclusive isolated-photon cross section
in pp collisions at √s = 13 TeV using 36 fb−1
of ATLAS data},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {10},
Year = {2019},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2019)203},
Abstract = {The differential cross section for isolated-photon
production in pp collisions is measured at a centre-of-mass
energy of 13 TeV with the ATLAS detector at the LHC using an
integrated luminosity of 36.1 fb−1. The differential cross
section is presented as a function of the photon transverse
energy in different regions of photon pseudorapidity. The
differential cross section as a function of the absolute
value of the photon pseudorapidity is also presented in
different regions of photon transverse energy.
Next-to-leading-order QCD calculations from Jetphox and
Sherpa as well as next-to-next-to-leading-order QCD
calculations from Nnlojet are compared with the measurement,
using several parameterisations of the proton parton
distribution functions. The predictions provide a good
description of the data within the experimental and
theoretical uncertainties. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2019)203},
Key = {fds356569}
}
@article{fds308112,
Author = {Abulencia, and A, and others},
Title = {Measurement of the inclusive jet cross section in ppbar
Interactions at sqrt{s}=1.96 TeV Using a Cone-based Jet
Algorithm},
Journal = {Phys. Rev.},
Volume = {D74},
Number = {7},
Pages = {071103},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.071103},
Abstract = {We present a measurement of the inclusive jet cross section
in ppbar interactions at sqrt{s}=1.96 TeV using 385 pb^{-1}
of data collected with the CDF II detector at the Fermilab
Tevatron. The results are obtained using an improved
cone-based jet algorithm (Midpoint). The data cover the jet
transverse momentum range from 61 to 620 GeV/c, extending
the reach by almost 150 GeV/c compared with previous
measurements at the Tevatron. The results are in good
agreement with next-to-leading order perturbative QCD
predictions using the CTEQ6.1M parton distribution
functions.},
Doi = {10.1103/PhysRevD.74.071103},
Key = {fds308112}
}
@article{fds308099,
Author = {Abulencia, and A, and others},
Title = {Measurement of the inclusive jet cross section using the
k(t) algorithm in p anti-p collisions at $\sqrt{s}=$ 1.96-
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {12},
Pages = {122001},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.122001},
Abstract = {We report on a measurement of the inclusive jet production
cross section in p anti-p collisions at s**(1/2) = 1.96 TeV
using data collected with the upgraded Collider Detector at
Fermilab in Run II (CDF II) corresponding to an integrated
luminosity of 385 pb-1. Jets are reconstructed using the K_T
algorithm. The measurement is carried out for jets with
rapidity $0.1},
Doi = {10.1103/physrevlett.96.122001},
Key = {fds308099}
}
@article{fds308075,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
MA},
Title = {Measurement of the inclusive jet cross section using the kT
algorithm in pp̄ collisions at s=1.96TeV with the CDF II
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {75},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.75.092006},
Abstract = {We report on measurements of the inclusive jet production
cross section as a function of the jet transverse momentum
in pp̄ collisions at s=1.96TeV, using the kT algorithm and
a data sample corresponding to 1.0fb-1 collected with the
Collider Detector at Fermilab in run II. The measurements
are carried out in five different jet rapidity regions with
|yjet|<2.1 and transverse momentum in the range
54<pTjet<700GeV/c. Next-to-leading order perturbative QCD
predictions are in good agreement with the measured cross
sections. © 2007 The American Physical Society.},
Doi = {10.1103/PhysRevD.75.092006},
Key = {fds308075}
}
@article{fds307588,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, KM and Blair,
RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A},
Title = {Measurement of the inclusive jet cross-section in pp
collisions at [Formula: see text] and comparison to the
inclusive jet cross-section at [Formula: see text] using the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {8},
Pages = {2509},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2509-4},
Abstract = {The inclusive jet cross-section has been measured in
proton-proton collisions at [Formula: see text] in a dataset
corresponding to an integrated luminosity of [Formula: see
text] collected with the ATLAS detector at the Large Hadron
Collider in 2011. Jets are identified using the
anti-<i>k</i><sub><i>t</i></sub> algorithm with two radius
parameters of 0.4 and 0.6. The inclusive jet
double-differential cross-section is presented as a function
of the jet transverse momentum <i>p</i><sub>T</sub> and jet
rapidity <i>y</i>, covering a range of 20≤<i>p</i><sub>T</sub><430 GeV
and |<i>y</i>|<4.4. The ratio of the cross-section to the
inclusive jet cross-section measurement at [Formula: see
text], published by the ATLAS Collaboration, is calculated
as a function of both transverse momentum and the
dimensionless quantity [Formula: see text], in bins of jet
rapidity. The systematic uncertainties on the ratios are
significantly reduced due to the cancellation of correlated
uncertainties in the two measurements. Results are compared
to the prediction from next-to-leading order perturbative
QCD calculations corrected for non-perturbative effects, and
next-to-leading order Monte Carlo simulation. Furthermore,
the ATLAS jet cross-section measurements at [Formula: see
text] and [Formula: see text] are analysed within a
framework of next-to-leading order perturbative QCD
calculations to determine parton distribution functions of
the proton, taking into account the correlations between the
measurements.},
Doi = {10.1140/epjc/s10052-013-2509-4},
Key = {fds307588}
}
@article{fds310305,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the inclusive jet cross-section in
proton-proton collisions at √s=7 TeV using 4.5
fb−1 of data with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {2},
Pages = {1-54},
Publisher = {Springer Nature},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2015)153},
Abstract = {Abstract: The inclusive jet cross-section is measured in
proton-proton collisions at a centre-of-mass energy of 7 TeV
using a data set corresponding to an integrated luminosity
of 4.5 fb−1 collected with the ATLAS detector at the Large
Hadron Collider in 2011. Jets are identified using the
anti-kt algorithm with radius parameter values of 0.4 and
0.6. The double-differential cross-sections are presented as
a function of the jet transverse momentum and the jet
rapidity, covering jet transverse momenta from 100 GeV to 2
TeV. Next-to-leading-order QCD calculations corrected for
non-perturbative effects and electroweak effects, as well as
Monte Carlo simulations with next-to-leading-order matrix
elements interfaced to parton showering, are compared to the
measured cross-sections. A quantitative comparison of the
measured cross-sections to the QCD calculations using
several sets of parton distribution functions is
performed.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP02(2015)153},
Key = {fds310305}
}
@article{fds356736,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Measurement of the inclusive jet cross-sections in
proton-proton collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {9},
Year = {2017},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2017)020},
Abstract = {Inclusive jet production cross-sections are measured in
proton-proton collisions at a centre-of-mass energy of s=8
TeV recorded by the ATLAS experiment at the Large Hadron
Collider at CERN. The total integrated luminosity of the
analysed data set amounts to 20.2 fb−1.
Double-differential cross-sections are measured for jets
defined by the anti-kt jet clustering algorithm with radius
parameters of R = 0.4 and R = 0.6 and are presented as a
function of the jet transverse momentum, in the range
between 70 GeV and 2.5 TeV and in six bins of the absolute
jet rapidity, between 0 and 3.0. The measured cross-sections
are compared to predictions of quantum chromodynamics,
calculated at next-to-leading order in perturbation theory,
and corrected for non-perturbative and electroweak effects.
The level of agreement with predictions, using a selection
of different parton distribution functions for the proton,
is quantified. Tensions between the data and the theory
predictions are observed.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP09(2017)020},
Key = {fds356736}
}
@article{fds310371,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Henry, S and Herndon,
M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta,
A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra,
A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of the inclusive leptonic asymmetry in top-quark
pairs that decay to two charged leptons at
CDF.},
Journal = {Physical review letters},
Volume = {113},
Number = {4},
Pages = {042001},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.113.042001},
Abstract = {We measure the inclusive forward-backward asymmetry of the
charged-lepton pseudorapidities from top-quark pairs
produced in proton-antiproton collisions and decaying to
final states that contain two charged leptons (electrons or
muons). The data are collected with the Collider Detector at
Fermilab and correspond to an integrated luminosity of 9.1
fb(-1). We measure the leptonic forward-backward asymmetry,
A(FB)(ℓ), to be 0.072 ± 0.060 and the leptonic pair
forward-backward asymmetry, A(FB)(ℓℓ), to be 0.076 ±
0.082. The measured values can be compared with the standard
model predictions of A(FB)(ℓ) = 0.038 ± 0.003 and
A(FB)(ℓℓ) = 0.048 ± 0.004, respectively. Additionally,
we combine the A(FB)(ℓ) result with a previous
determination from a final state with a single lepton and
hadronic jets and obtain A(FB)(ℓ) = 0.090(-0.026)(+0.028).},
Doi = {10.1103/physrevlett.113.042001},
Key = {fds310371}
}
@article{fds307742,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the inclusive W± and Z/γ∗
cross sections in the e and μ decay channels in pp
collisions at √s=7TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.85.072004},
Abstract = {The production cross sections of the inclusive Drell-Yan
processes W ±→ν and Z/γ∗→(=e, μ) are measured in
proton-proton collisions at √s=7TeV with the ATLAS
detector. The cross sections are reported integrated over a
fiducial kinematic range, extrapolated to the full range,
and also evaluated differentially as a function of the W
decay lepton pseudorapidity and the Z boson rapidity,
respectively. Based on an integrated luminosity of about
35pb-1 collected in 2010, the precision of these
measurements reaches a few percent. The integrated and the
differential W± and Z/γ∗ cross sections in the e and μ
channels are combined, and compared with perturbative QCD
calculations, based on a number of different parton
distribution sets available at next-to-next-to-leading
order.},
Doi = {10.1103/PhysRevD.85.072004},
Key = {fds307742}
}
@article{fds356722,
Author = {Aaltonen, T and Albrow, MG and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri,
A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto and A and Di Ruzza,
B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Erbacher, R and Errede,
S},
Title = {Measurement of the inclusive-isolated prompt-photon cross
section in pp collisions using the full CDF data
set},
Journal = {Physical Review D},
Volume = {96},
Number = {9},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.96.092003},
Abstract = {A measurement of the inclusive production cross section of
isolated prompt photons in proton-antiproton collisions at
center-of-mass energy s=1.96 TeV is presented. The results
are obtained using the full Run II data sample collected
with the Collider Detector at the Fermilab Tevatron, which
corresponds to an integrated luminosity of 9.5 fb-1. The
cross section is measured as a function of photon transverse
energy, ETγ, in the range 30<ETγ<500 GeV and in the
pseudorapidity region |ηγ|<1.0. The results are compared
with predictions from parton-shower Monte Carlo models at
leading order in QCD and from next-to-leading-order
perturbative QCD calculations. The latter show good
agreement with the measured cross section.},
Doi = {10.1103/PhysRevD.96.092003},
Key = {fds356722}
}
@article{fds321080,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Measurement of the Inelastic Proton-Proton Cross Section at
sqrt[s]=13 TeV with the ATLAS Detector at the
LHC.},
Journal = {Phys Rev Lett},
Volume = {117},
Number = {18},
Pages = {182002},
Year = {2016},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevLett.117.182002},
Abstract = {This Letter presents a measurement of the inelastic
proton-proton cross section using 60 μb^{-1} of pp
collisions at a center-of-mass energy sqrt[s] of 13 TeV
with the ATLAS detector at the LHC. Inelastic interactions
are selected using rings of plastic scintillators in the
forward region (2.07<|η|<3.86) of the detector. A cross
section of 68.1±1.4 mb is measured in the fiducial
region ξ=M_{X}^{2}/s>10^{-6}, where M_{X} is the larger
invariant mass of the two hadronic systems separated by the
largest rapidity gap in the event. In this ξ range the
scintillators are highly efficient. For diffractive events
this corresponds to cases where at least one proton
dissociates to a system with M_{X}>13 GeV. The measured
cross section is compared with a range of theoretical
predictions. When extrapolated to the full phase space, a
cross section of 78.1±2.9 mb is measured, consistent
with the inelastic cross section increasing with
center-of-mass energy.},
Doi = {10.1103/PhysRevLett.117.182002},
Key = {fds321080}
}
@article{fds321140,
Author = {ATLAS Collaboration},
Title = {Measurement of the inelastic proton-proton cross-section at
√s=7 TeV with the ATLAS detector.},
Journal = {Nature communications},
Volume = {2},
Number = {1},
Pages = {463},
Year = {2011},
Month = {September},
url = {http://dx.doi.org/10.1038/ncomms1472},
Abstract = {The dependence of the rate of proton-proton interactions on
the centre-of-mass collision energy, √s, is of fundamental
importance for both hadron collider physics and particle
astrophysics. The dependence cannot yet be calculated from
first principles; therefore, experimental measurements are
needed. Here we present the first measurement of the
inelastic proton-proton interaction cross-section at a
centre-of-mass energy, √s, of 7 TeV using the ATLAS
detector at the Large Hadron Collider. Events are selected
by requiring hits on scintillation counters mounted in the
forward region of the detector. An inelastic cross-section
of 60.3 ± 2.1 mb is measured for ξ > 5×10⁻⁶, where ξ
is calculated from the invariant mass, M(X), of hadrons
selected using the largest rapidity gap in the event. For
diffractive events, this corresponds to requiring at least
one of the dissociation masses to be larger than 15.7
GeV.},
Doi = {10.1038/ncomms1472},
Key = {fds321140}
}
@article{fds307744,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Measurement of the isolated diphoton cross section in pp
collisions at √s=7TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012003},
Abstract = {The ATLAS experiment has measured the production cross
section of events with two isolated photons in the final
state, in proton-proton collisions at √s=7TeV. The full
data set acquired in 2010 is used, corresponding to an
integrated luminosity of 37pb -1. The background, consisting
of hadronic jets and isolated electrons, is estimated with
fully data-driven techniques and subtracted. The
differential cross sections, as functions of the di-photon
mass (m γγ), total transverse momentum (p T,γγ), and
azimuthal separation (Δφ γγ), are presented and compared
to the predictions of next-to-leading-order QCD. © 2012
CERN.},
Doi = {10.1103/PhysRevD.85.012003},
Key = {fds307744}
}
@article{fds340913,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
L and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and DrollingerV, and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, V and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and HaywardH, and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and HoffmanK, D and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen,
D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
D},
Title = {Measurement of the J/ψ meson and b-hadron production cross
sections in pp̄ collisions at √s = 1960
GeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {3},
Pages = {032001-1-032001-26},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.032001},
Abstract = {We present a new measurement of the inclusive and
differential production cross sections of J/ψ mesons and b
hadrons in proton-antiproton collisions at √s = 1960 GeV.
The data correspond to an integrated luminosity of 39.7 pb-1
collected by the CDF run II detector. We find the integrated
cross section for inclusive J/ψ production for all
transverse momenta from 0 to 20 GeV/c in the rapidity range
|y| < 0.6 to be 4.08 ± 0.02(Stat)-0.33+0.36(syst) μb.
We separate the fraction of J/ψ events from the decay of
the long-lived b hadrons using the lifetime distribution in
all events with pT(J/ψ) > 1.25 GeV/c. We find the total
cross section for b hadrons, including both hadrons and
antihadrons, decaying to J/ψ with transverse momenta
greater than 1.25 GeV/c in the rapidity range |y(J/ψ)| <
0.6 is 0.330 ± 0.005(stat) -0.033+0.036(syst) μb. Using a
Monte Carlo simulation of the decay kinematics of b hadrons
to all final states containing a J/ψ, we extract the first
measurement of the total single b-hadron cross section down
to zero transverse momentum at √s = 1960 GeV. We find the
total single b-hadron cross section integrated over all
transverse momenta for b hadrons in the rapidity range |y|
< 0.6 to be 17.6 ± 0.4(stat) -2.3+2.5(syst) μb. © 2005
The American Physical Society.},
Doi = {10.1103/PhysRevD.71.032001},
Key = {fds340913}
}
@article{fds310408,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the jet fragmentation function and transverse
profile in proton–proton collisions at a center-of-mass
energy of 7 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {71},
Number = {11},
Publisher = {Springer Nature},
Year = {2011},
Month = {December},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1795-y},
Abstract = {The jet fragmentation function and transverse profile for
jets with 25 GeV< pTjet < 500 GeV and |ηjet| < 1.2 produced
in proton–proton collisions with a center-ofmass energy of
7 TeV are presented. The measurement is performed using data
with an integrated luminosity of 36 pb−1. Jets are
reconstructed and their momentum measured using calorimetric
information. The momenta of the charged particle
constituents are measured using the tracking system. The
distributions corrected for detector effects are compared
with various Monte Carlo event generators and generator
tunes. Several of these choices show good agreement with the
measured fragmentation function. None of these choices
reproduce both the transverse profile and fragmentation
function over the full kinematic range of the
measurement.},
Doi = {10.1140/epjc/s10052-011-1795-y},
Key = {fds310408}
}
@article{fds307626,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, R and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, E and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, R and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
M and Belloni, A and Belaboradova, O and Belotiskiy, K and Beltramello,
O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Nocioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Bensalma, K and Bentvelsen, S and Berge,
D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitnec, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boviea, A and Boyd, J and Boyka, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, E and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Carbreara Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
MDMC and Caprini, I and Caprini, M and Capriotti, D and Capau, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, E and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, E and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
NJ and Collins-Tooth, C and Collot, J},
Title = {Measurement of the jet radius and transverse momentum
dependence of inclusive jet suppression in lead-lead
collisions at √SNN=2.76 TeV with the
ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {719},
Number = {4-5},
Pages = {220-241},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.024},
Abstract = {Measurements of inclusive jet suppression in heavy ion
collisions at the LHC provide direct sensitivity to the
physics of jet quenching. In a sample of lead–lead
collisions at sNN=2.76 TeV corresponding to an integrated
luminosity of approximately 7 μb−1, ATLAS has measured
jets with a calorimeter system over the pseudorapidity
interval |η|<2.1 and over the transverse momentum range
38<pT<210 GeV. Jets were reconstructed using the anti-kt
algorithm with values for the distance parameter that
determines the nominal jet radius of R=0.2, 0.3, 0.4 and
0.5. The centrality dependence of the jet yield is
characterized by the jet “central-to-peripheral ratio,”
RCP. Jet production is found to be suppressed by
approximately a factor of two in the 10% most central
collisions relative to peripheral collisions. RCP varies
smoothly with centrality as characterized by the number of
participating nucleons. The observed suppression is only
weakly dependent on jet radius and transverse momentum.
These results provide the first direct measurement of
inclusive jet suppression in heavy ion collisions and
complement previous measurements of dijet transverse energy
imbalance at the LHC.},
Doi = {10.1016/j.physletb.2013.01.024},
Key = {fds307626}
}
@article{fds356744,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Measurement of the k t splitting scales in Z →
ℓℓ events in pp collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {8},
Year = {2017},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2017)026},
Abstract = {A measurement of the splitting scales occuring in the kt
jet-clustering algorithm is presented for final states
containing a Z boson. The measurement is done using 20.2
fb−1 of proton-proton collision data collected at a
centre-of-mass energy of s=8 TeV by the ATLAS experiment at
the LHC in 2012. The measurement is based on chargedparticle
track information, which is measured with excellent
precision in the pT region relevant for the transition
between the perturbative and the non-perturbative regimes.
The data distributions are corrected for detector effects,
and are found to deviate from state-of-the-art predictions
in various regions of the observables.[Figure not available:
see fulltext.].},
Doi = {10.1007/JHEP08(2017)026},
Key = {fds356744}
}
@article{fds307950,
Author = {Aaltonen, T and others},
Title = {Measurement of the k[sub T] Distribution of Particles in
Jets Produced in p[overline p] Collisions at sqrt(s) = 1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {23},
Pages = {232002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.232002},
Abstract = {We present a measurement of the transverse momentum with
respect to the jet axis (k(t)) of particles in jets produced
in pp collisions at sqrt(s)=1.96 TeV. Results are obtained
for charged particles in a cone of 0.5 radians around the
jet axis in events with dijet invariant masses between 66
and 737 GeV/c(2). The experimental data are compared to
theoretical predictions obtained for fragmentation partons
within the framework of resummed perturbative QCD using the
modified leading log and next-to-modified leading log
approximations. The comparison shows that trends in data are
successfully described by the theoretical predictions,
indicating that the perturbative QCD stage of jet
fragmentation is dominant in shaping basic jet
characteristics.},
Doi = {10.1103/physrevlett.102.232002},
Key = {fds307950}
}
@article{fds307569,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Measurement of the leptonic asymmetry in tt̄ events
produced in pp̄ collisions at √s=1.96
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.072003},
Abstract = {We measure the asymmetry in the charge-weighted rapidity
qyℓ of the lepton in semileptonic tt̄ decays recorded
with the CDF II detector using the full Tevatron Run II
sample, corresponding to an integrated luminosity of 9.4
fb-1. A parametrization of the asymmetry as a function of
qyℓ is used to correct for the finite acceptance of the
detector and recover the production-level asymmetry. The
result of AFBℓ=0.094-0.029+0.032 is to be compared to the
standard model next-to-leading-order prediction of
AFBℓ=0.038±0.003. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.072003},
Key = {fds307569}
}
@article{fds308133,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann,
JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko,
I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and da Costa, JG and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko,
I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann,
SE and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu,
R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller,
L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes,
C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti,
R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompos, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
D},
Title = {Measurement of the lifetime difference between Bs mass
eigenstates.},
Journal = {Physical review letters},
Volume = {94},
Number = {10},
Pages = {101803},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.94.101803},
Abstract = {We present measurements of the lifetimes and polarization
amplitudes for B(0)(s)-->J/psiphi and B(0)(d)-->J/psiK(*0)
decays. Lifetimes of the heavy and light mass eigenstates in
the B(0)(s) system are separately measured for the first
time by determining the relative contributions of amplitudes
with definite CP as a function of the decay time. Using
203+/-15 B(0)(s) decays we obtain tau(L) =
(1.05(+0.16)(-0.13) +/- 0.02) ps and tau(H) =
(2.07(+0.58)(-0.46) +/- 0.03) ps. Expressed in terms of the
difference DeltaGamma(s) and average Gamma(s), of the decay
rates of the two eigenstates, the results are
DeltaGamma(s)/Gamma(s) = (65(+25)(-33) +/- 1)% and
DeltaGamma(s) = (0.47(+0.19)(-0.24) +/- 0.01)
ps(-1).},
Doi = {10.1103/physrevlett.94.101803},
Key = {fds308133}
}
@article{fds310376,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurement of the low-mass Drell-Yan differential cross
section at √s = 7 TeV using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {6},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2014)112},
Abstract = {The differential cross section for the process Z/γ * →
ℓℓ (ℓ = e, μ) as a function of dilepton invariant
mass is measured in pp collisions at √s = 7 TeV at the LHC
using the ATLAS detector. The measurement is performed in
the e and μ channels for invariant masses between 26 GeV
and 66 GeV using an integrated luminosity of 1.6 fb -1
collected in 2011 and these measurements are combined. The
analysis is extended to invariant masses as low as 12 GeV in
the muon channel using 35 pb-1 of data collected in 2010.
The cross sections are determined within fiducial acceptance
regions and corrections to extrapolate the measurements to
the full kinematic range are provided. Next-to-next-to-leading-
order QCD predictions provide a significantly better
description of the results than next-to-leading-order QCD
calculations, unless the latter are matched to a parton
shower calculation. [Figure not available: see fulltext.] ©
2014 The Author(s).},
Doi = {10.1007/JHEP06(2014)112},
Key = {fds310376}
}
@article{fds350337,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Artz,
S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Avramidou,
R and Ayoub, MK and Azoulay, AM and Azuelos, G and Bachacou, H and Bachas,
K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura,
AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Barsov, S and Bartoldus, R and Bartolini,
G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat,
A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool,
B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertram, IA and Bessidskaia Bylund and O and Besson,
N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai, P and Bi, R and Bianchi, RM and Biebel,
O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton,
CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans,
R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero,
J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carter, JWS and Casado, MP and Casha,
AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni,
V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen,
J and Chen, S and Chen, SJ and Chen, X and Chen, Y-H and Cheng, HC and Cheng,
HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, YS and Chu, MC and Chu, X and Chudoba, J and Chuinard, AJ and Chwastowski, JJ},
Title = {Measurement of the Lund Jet Plane Using Charged Particles in
13 TeV Proton-Proton Collisions with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {124},
Number = {22},
Pages = {222002},
Year = {2020},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.124.222002},
Abstract = {The prevalence of hadronic jets at the LHC requires that a
deep understanding of jet formation and structure is
achieved in order to reach the highest levels of
experimental and theoretical precision. There have been many
measurements of jet substructure at the LHC and previous
colliders, but the targeted observables mix physical effects
from various origins. Based on a recent proposal to
factorize physical effects, this Letter presents a
double-differential cross-section measurement of the Lund
jet plane using 139 fb^{-1} of sqrt[s]=13 TeV
proton-proton collision data collected with the ATLAS
detector using jets with transverse momentum above 675 GeV.
The measurement uses charged particles to achieve a fine
angular resolution and is corrected for acceptance and
detector effects. Several parton shower Monte Carlo models
are compared with the data. No single model is found to be
in agreement with the measured data across the entire
plane.},
Doi = {10.1103/physrevlett.124.222002},
Key = {fds350337}
}
@article{fds307849,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the Mass Difference between $t$ and
$\overline{t}$ Quarks},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {15},
Pages = {152001},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.152001},
Abstract = {We present a direct measurement of the mass difference
between t and t quarks using tt candidate events in the
lepton+jets channel, collected with the CDF II detector at
Fermilab's 1.96 TeV Tevatron pp Collider. We make an event
by event estimate of the mass difference to construct
templates for top quark pair signal events and background
events. The resulting mass difference distribution of data
is compared to templates of signals and background using a
maximum likelihood fit. From a sample corresponding to an
integrated luminosity of 5.6 fb(-1), we measure a mass
difference, ΔM(top) = M(t) - M(t) = -3.3 ± 1.4(stat) ±
1.0(syst) GeV/c2, approximately 2 standard deviations
away from the CPT hypothesis of zero mass
difference.},
Doi = {10.1103/PhysRevLett.106.152001},
Key = {fds307849}
}
@article{fds307554,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
JF},
Title = {Measurement of the mass difference between top and anti-top
quarks in pp collisions at √s=7 TeV using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {728},
Pages = {363-379},
Publisher = {Elsevier BV},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2013.12.010},
Abstract = {A measurement of the mass difference between top and
anti-top quarks is presented. In a 4.7 fb−1 data sample of
proton–proton collisions at s=7 TeV recorded with the
ATLAS detector at the LHC, events consistent with tt¯
production and decay into a single charged lepton final
state are reconstructed. For each event, the mass difference
between the top and anti-top quark candidate is calculated.
A two b-tag requirement is used in order to reduce the
background contribution. A maximum likelihood fit to these
per-event mass differences yields Δm≡mt−mt¯=0.67±0.61(stat)±0.41(syst)
GeV, consistent with CPT invariance.},
Doi = {10.1016/j.physletb.2013.12.010},
Key = {fds307554}
}
@article{fds307680,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and Barbaro,
PD and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Canto,
AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Ramos, JPF and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Garfinkel, AF and Garosi,
P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and López, OG and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare,
M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim,
JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata,
M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino,
G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani,
A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov,
A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Fernández, IR and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov,
A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, WM and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S},
Title = {Measurement of the mass difference between top and antitop
quarks},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {5},
Pages = {052013},
Year = {2013},
url = {http://dx.doi.org/10.1103/PhysRevD.87.052013},
Abstract = {We present a measurement of the mass difference between top
(t) and antitop (t̄) quarks using tt̄ candidate events
reconstructed in the final state with one lepton and
multiple jets. We use the full data set of Tevatron
√s=1.96 TeV proton-antiproton collisions recorded by the
CDF II detector, corresponding to an integrated luminosity
of 8.7 fb-1. We estimate event by event the mass difference
to construct templates for top pair signal events and
background events. The resulting mass difference
distribution in data compared to signal and background
templates using a likelihood fit yields ΔMtop=Mt-Mt̄=-1.95±1.11(stat)
±0.59(syst) GeV/c2 and is in agreement with the standard
model prediction of no mass difference. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.87.052013},
Key = {fds307680}
}
@article{fds331626,
Author = {Collaboration, DAEACDF},
Title = {Measurement of the mass difference m(D+s)-m(D+) at CDF
II},
Journal = {Physical Review},
Volume = {D68},
Number = {7},
Pages = {072004},
Publisher = {American Physical Society (APS)},
Year = {2003},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.68.072004},
Abstract = {We present a measurement of the mass difference
m(D+s)-m(D+), where both the D+s and D+ are reconstructed in
the phi pi + decay channel. This measurement uses 11.6 pb-1
of data collected by CDF II using the new displaced-track
trigger. The mass difference is found to bem(D+s)-
m(D+)=99.41±0.38(stat)±0.21(syst) MeV/c2.},
Doi = {10.1103/PhysRevD.68.072004},
Key = {fds331626}
}
@article{fds307802,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli,
M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F and D'errico, M and Di Canto,
A},
Title = {Measurement of the masses and widths of the bottom baryons
Σb± and Σb*±},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.85.092011},
Abstract = {Using data from pp̄ collisions at √s=1.96TeV recorded by
the CDF II detector at the Fermilab Tevatron, we present
improved measurements of the masses and first measurements
of natural widths of the four bottom baryon resonance states
Σb+, Σb*+ and Σb-, Σb*-. These states are fully
reconstructed in their decay modes to Λb0π ± where
Λb0→Λc+π - with Λc+→pK -π +. The analysis is based
on a data sample corresponding to an integrated luminosity
of 6.0fb -1 collected by an online event selection based on
tracks displaced from the pp̄ interaction point. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.092011},
Key = {fds307802}
}
@article{fds323243,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Dörr, C and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ehlers, J and Ely, R and Erbacher, R and Erdmann, M and Errede,
D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko,
I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein,
E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher,
F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang,
D and Jarrell, J and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo,
KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin,
PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King,
BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Mehta, A and Menzemer,
S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao,
T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel,
R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PAM and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa,
T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman,
MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert,
B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert,
K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu,
V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri,
F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF},
Title = {Measurement of the moments of the hadronic invariant mass
distribution in semileptonic B decays},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {5},
Pages = {1-9},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.051103},
Abstract = {Using 180 pb -1 of data collected with the CDF II detector
at the Tevatron, we measure the first two moments of the
hadronic invariant mass-squared distribution in charmed
semileptonic B decays. From these we determine the
nonperturbative Heavy Quark Effective Theory parameters Λ
and λ 1 used to relate the B meson semileptonic branching
ratio to the CKM matrix element |V cb|. For a minimum lepton
momentum of 0.7 GeV/c in the B rest frame we measure the
first two moments of the D** → D (*)π component to be
〈m D**2〉 = (5.83 ± 0.16 stat ± 0.08 syst) GeV 2/c 4
and 〈(m D**2 - 〈m D**2〉) 2〉 = (1.30 ± 0.69 stat ±
0.22 syst) GeV 4/c 8. Combining these with the discrete mass
terms from the D and D* mesons, we find the total moments to
be 〈M Ξc2〉 - m̄ D2 = (0.467 ± 0.038 stat ± 0.068
syst GeV 2/c 4 and 〈(M Ξc2 - 〈M Ξc2〉) 2〉 = (1.05
± 0.26 stat ± 0.13 syst) GeV 4/c 8, where m̄ D is the
spin-averaged D mass. The systematic error is dominated by
the uncertainties in the world-average branching ratios used
to combine the D, D*, and D** contributions. The analysis
makes no assumptions about the shape or resonant structure
of the D** → D (*)π invariant mass distribution. © 2005
The American Physical Society.},
Doi = {10.1103/PhysRevD.71.051103},
Key = {fds323243}
}
@article{fds310390,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, M and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Measurement of the muon reconstruction performance of the
ATLAS detector using 2011 and 2012 LHC proton-proton
collision data.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {11},
Pages = {3130},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3130-x},
Abstract = {This paper presents the performance of the ATLAS muon
reconstruction during the LHC run with [Formula: see text]
collisions at [Formula: see text]-8 TeV in 2011-2012,
focusing mainly on data collected in 2012. Measurements of
the reconstruction efficiency and of the momentum scale and
resolution, based on large reference samples of [Formula:
see text], [Formula: see text] and [Formula: see text]
decays, are presented and compared to Monte Carlo
simulations. Corrections to the simulation, to be used in
physics analysis, are provided. Over most of the covered
phase space (muon [Formula: see text] and [Formula: see
text] GeV) the efficiency is above [Formula: see text] and
is measured with per-mille precision. The momentum
resolution ranges from [Formula: see text] at central
rapidity and for transverse momentum [Formula: see
text] GeV, to [Formula: see text] at large rapidity and
[Formula: see text] GeV. The momentum scale is known with
an uncertainty of [Formula: see text] to [Formula: see text]
depending on rapidity. A method for the recovery of final
state radiation from the muons is also presented.},
Doi = {10.1140/epjc/s10052-014-3130-x},
Key = {fds310390}
}
@article{fds347445,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Measurement of the nuclear modification factor for inclusive
jets in Pb+Pb collisions at √sNN=5.02 TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {790},
Pages = {108-128},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2018.10.076},
Abstract = {Measurements of the yield and nuclear modification factor,
RAA, for inclusive jet production are performed using 0.49
nb−1 of Pb+Pb data at sNN=5.02TeV and 25 pb−1 of Pb+Pb
data at s=5.02TeV with the ATLAS detector at the LHC. Jets
are reconstructed with the anti-kt algorithm with radius
parameter R=0.4 and are measured over the transverse
momentum range of 40–1000 GeV in six rapidity intervals
covering |y|<2.8. The magnitude of RAA increases with
increasing jet transverse momentum, reaching a value of
approximately 0.6 at 1 TeV in the most central collisions.
The magnitude of RAA also increases towards peripheral
collisions. The value of RAA is independent of rapidity at
low jet transverse momenta, but it is observed to decrease
with increasing rapidity at high transverse
momenta.},
Doi = {10.1016/j.physletb.2018.10.076},
Key = {fds347445}
}
@article{fds371118,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Measurement of the nuclear modification factor of b-jets in
5.02 TeV Pb+Pb collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11427-9},
Abstract = {This paper presents a measurement of b-jet production in
Pb+Pb and pp collisions at sNN=5.02 TeV with the ATLAS
detector at the LHC. The measurement uses 260 pb - 1 of pp
collisions collected in 2017 and 1.4 nb - 1 of Pb+Pb
collisions collected in 2018. In both collision systems,
jets are reconstructed via the anti- kt algorithm. The
b-jets are identified from a sample of jets containing muons
from the semileptonic decay of b-quarks using template fits
of the muon momentum relative to the jet axis. In pp
collisions, b-jets are reconstructed for radius parameters
R= 0.2 and R= 0.4 , and only R= 0.2 jets are used in Pb+Pb
collisions. For comparison, inclusive R= 0.2 jets are also
measured using 1.7 nb - 1 of Pb+Pb collisions collected in
2018 and the same pp collision data as the b-jet
measurement. The nuclear modification factor, RAA , is
calculated for both b-jets and inclusive jets with R= 0.2
over the transverse momentum range of 80–290 GeV. The
nuclear modification factor for b-jets decreases from
peripheral to central collisions. The ratio of the b-jet RAA
to inclusive jet RAA is also presented and suggests that the
RAA for b-jets is larger than that for inclusive jets in
central Pb+Pb collisions. The measurements are compared with
theoretical calculations and suggest a role for mass and
colour-charge effects in partonic energy loss in heavy-ion
collisions.},
Doi = {10.1140/epjc/s10052-023-11427-9},
Key = {fds371118}
}
@article{fds307538,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Measurement of the parity-violating asymmetry parameter αb
and the helicity amplitudes for the decay Λb0 →j /ψ Λ0
with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.89.092009},
Abstract = {A measurement of the parity-violating decay asymmetry
parameter, αb, and the helicity amplitudes for the decay
Λb0→J/ψ(μ+μ-)Λ0(pπ-) is reported. The analysis is
based on 1400 Λb0 and Λ¯b0 baryons selected in 4.6 fb-1
of proton-proton collision data with a center-of-mass energy
of 7 TeV recorded by the ATLAS experiment at the LHC. By
combining the Λb0 and Λ¯b0 samples under the assumption
of CP conservation, the value of αb is measured to be
0.30±0.16(stat)±0.06(syst). This measurement provides a
test of theoretical models based on perturbative QCD or
heavy-quark effective theory.},
Doi = {10.1103/PhysRevD.89.092009},
Key = {fds307538}
}
@article{fds356618,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos, SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Aperio Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz, V and Araujo Pereira, R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the photon identification efficiencies with
the ATLAS detector using LHC Run 2 data collected in 2015
and 2016},
Journal = {European Physical Journal C},
Volume = {79},
Number = {3},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6650-6},
Abstract = {The efficiency of the photon identification criteria in the
ATLAS detector is measured using 36.1fb1 to 36.7fb1 of pp
collision data at s=13 TeV collected in 2015 and 2016. The
efficiencies are measured separately for converted and
unconverted isolated photons, in four different
pseudorapidity regions, for transverse momenta between 10
GeV and 1.5 TeV. The results from the combination of three
data-driven techniques are compared with the predictions
from simulation after correcting the variables describing
the shape of electromagnetic showers in simulation for the
average differences observed relative to data.
Data-to-simulation efficiency ratios are determined to
account for the small residual efficiency differences. These
factors are measured with uncertainties between 0.5% and 5%
depending on the photon transverse momentum and
pseudorapidity. The impact of the isolation criteria on the
photon identification efficiency, and that of additional
soft pp interactions, are also discussed. The probability of
reconstructing an electron as a photon candidate is measured
in data, and compared with the predictions from simulation.
The efficiency of the reconstruction of photon conversions
is measured using a sample of photon candidates from Z→
μμγ events, exploiting the properties of the ratio of the
energies deposited in the first and second longitudinal
layers of the ATLAS electromagnetic calorimeter.},
Doi = {10.1140/epjc/s10052-019-6650-6},
Key = {fds356618}
}
@article{fds322003,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Measurement of the photon identification efficiencies with
the ATLAS detector using LHC Run-1 data.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {12},
Pages = {666},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4507-9},
Abstract = {The algorithms used by the ATLAS Collaboration to
reconstruct and identify prompt photons are described.
Measurements of the photon identification efficiencies are
reported, using 4.9 fb[Formula: see text] of pp collision
data collected at the LHC at [Formula: see text] [Formula:
see text] and 20.3 fb[Formula: see text] at [Formula: see
text] [Formula: see text]. The efficiencies are measured
separately for converted and unconverted photons, in four
different pseudorapidity regions, for transverse momenta
between 10 [Formula: see text] and 1.5 [Formula: see
text]. The results from the combination of three data-driven
techniques are compared to the predictions from a simulation
of the detector response, after correcting the
electromagnetic shower momenta in the simulation for the
average differences observed with respect to data.
Data-to-simulation efficiency ratios used as correction
factors in physics measurements are determined to account
for the small residual efficiency differences. These factors
are measured with uncertainties between 0.5% and 10% in
7 [Formula: see text] data and between 0.5% and 5.6% in
8 [Formula: see text] data, depending on the photon
transverse momentum and pseudorapidity.},
Doi = {10.1140/epjc/s10052-016-4507-9},
Key = {fds322003}
}
@article{fds372121,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez
Fernandez, A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH},
Title = {Measurement of the polarisation of W bosons produced in
top-quark decays using dilepton events at s=13 TeV with the
ATLAS experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137829},
Abstract = {A measurement of the polarisation of W bosons produced in
top-quark decays is presented, using proton–proton
collision data at a centre-of-mass energy of s=13 TeV. The
data were collected by the ATLAS detector at the Large
Hadron Collider and correspond to an integrated luminosity
of 139 fb−1. The measurement is performed selecting tt¯
events decaying into final states with two charged leptons
(electrons or muons) and at least two b-tagged jets. The
polarisation is extracted from the differential
cross-section distribution of the cosθ⁎ variable,
where θ⁎ is the angle between the momentum direction of
the charged lepton from the W boson decay and the reversed
momentum direction of the b-quark from the top-quark decay,
both calculated in the W boson rest frame. Parton-level
results, corrected for the detector acceptance and
resolution, are presented for the cosθ⁎ angle. The
measured fractions of longitudinal, left- and right-handed
polarisation states are found to be f0=0.684±0.005(stat.)±0.014(syst.),
fL=0.318±0.003(stat.)±0.008(syst.) and
fR=−0.002±0.002(stat.)±0.014(syst.), in agreement with
the Standard Model prediction.},
Doi = {10.1016/j.physletb.2023.137829},
Key = {fds372121}
}
@article{fds307725,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the polarisation of W bosons produced with
large transverse momentum in pp collisions at √s =7 TeV
with the ATLAS experiment},
Journal = {European Physical Journal C},
Volume = {72},
Number = {5},
Pages = {1-30},
Publisher = {Springer Nature},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2001-6},
Abstract = {This paper describes an analysis of the angular distribution
of W→eν and W→μν decays, using data from pp
collisions at √s =7 TeV recorded with the ATLAS detector
at the LHC in 2010, corresponding to an integrated
luminosity of about 35 pb-1. Using the decay lepton
transverse momentum and the missing transverse momentum, the
W decay angular distribution projected onto the transverse
plane is obtained and analysed in terms of helicity
fractions f0, fL and fR over two ranges of W transverse
momentum (pWT): 35 < pWT < 50 GeV and pWT > 50 GeV. Good
agreement is found with theoretical predictions. For pWT >50
GeV, the values of f0 and fL-fR, averaged over charge and
lepton flavour, are measured to be: f0=0. 127±0. 030±0.
108 and fL-fR=0. 252±0. 017±0. 030, where the first
uncertainties are statistical, and the second include all
systematic effects. © 2012 CERN for the benefit of the
ATLAS collaboration.},
Doi = {10.1140/epjc/s10052-012-2001-6},
Key = {fds307725}
}
@article{fds310282,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of the production and differential cross
sections of W+W- bosons in association
with jets in pp¯ collisions at √s = 1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.91.111101},
Abstract = {We present a measurement of the W-boson-pair production
cross section in pp¯ collisions at 1.96 TeV center-of-mass
energy and the first measurement of the differential cross
section as a function of jet multiplicity and leading-jet
energy. The W+W- cross section is measured in the final
state comprising two charged leptons and neutrinos, where
either charged lepton can be an electron or a muon. Using
data collected by the CDF experiment corresponding to
9.7fb-1 of integrated luminosity, a total of 3027 collision
events consistent with W+W- production are observed with an
estimated background contribution of 1790 ± 190 events. The
measured total cross section is σ(pp¯ → W+W-)= 14.0 ±
0.6 (stat)-1.0+1.2 (syst) ± 0.8 (lumi) pb, consistent with
the standard model prediction.},
Doi = {10.1103/PhysRevD.91.111101},
Key = {fds310282}
}
@article{fds356561,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V},
Title = {Measurement of the production cross section for a Higgs
boson in association with a vector boson in the
H → WW⁎ → ℓνℓν channel in pp
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {798},
Year = {2019},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2019.134949},
Abstract = {A measurement of the Higgs boson production cross sections
via associated WH and ZH production using
H→WW⁎→ℓνℓν decays, where ℓ stands for either
an electron or a muon, is presented. Results for combined WH
and ZH production are also presented. The analysis uses
events produced in proton–proton collisions collected with
the ATLAS detector at the Large Hadron Collider in 2015 and
2016. The data correspond to an integrated luminosity of
36.1fb−1 recorded at a centre-of-mass energy of 13 TeV.
The products of the H→WW⁎ branching fraction times the
WH and ZH cross sections are measured to be
0.67−0.27+0.31(stat.)−0.14+0.18(syst.) pb and
0.54−0.24+0.31(stat.)−0.07+0.15(syst.) pb respectively,
in agreement with the Standard Model predictions.},
Doi = {10.1016/j.physletb.2019.134949},
Key = {fds356561}
}
@article{fds307757,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the production cross section for Z/γ* in
association with jets in pp collisions at √s=7TeV with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.85.032009},
Abstract = {Results are presented on the production of jets of particles
in association with a Z/γ* boson, in proton-proton
collisions at √s=7TeV with the ATLAS detector. The
analysis includes the full 2010 data set, collected with a
low rate of multiple proton-proton collisions in the
accelerator, corresponding to an integrated luminosity of
36pb-1. Inclusive jet cross sections in Z/γ* events, with
Z/γ* decaying into electron or muon pairs, are measured for
jets with transverse momentum pT>30GeV and jet rapidity
|y|<4.4. The measurements are compared to
next-to-leading-order perturbative QCD calculations, and to
predictions from different Monte Carlo generators
implementing leading-order matrix elements supplemented by
parton showers. © 2012 CERN.},
Doi = {10.1103/PhysRevD.85.032009},
Key = {fds307757}
}
@article{fds307736,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the production cross section of an isolated
photon associated with jets in proton-proton collisions at
√s=7TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.85.092014},
Abstract = {A measurement of the cross section for the production of an
isolated photon in association with jets in proton-proton
collisions at a center-of-mass energy √s=7TeV is
presented. Photons are reconstructed in the pseudorapidity
range |ηγ|<1.37 and with a transverse energy ETγ>25GeV.
Jets are reconstructed in the rapidity range |yjet|<4.4 and
with a transverse momentum pTjet>20GeV. The differential
cross section dσ/dETγ is measured, as a function of the
photon transverse energy, for three different rapidity
ranges of the leading-pT jet: |yjet|<1.2, 1.2≤|yjet|<2.8
and 2.8≤|yjet|<4.4. For each rapidity configuration the
same-sign (ηγyjet 0) and opposite-sign (ηγyjet<0) cases
are studied separately. The results are based on an
integrated luminosity of 37pb-1, collected with the ATLAS
detector at the LHC. Next-to-leading order perturbative QCD
calculations are found to be in fair agreement with the
data, except for ETγ 45GeV, where the theoretical
predictions overestimate the measured cross sections. ©
2012 CERN.},
Doi = {10.1103/PhysRevD.85.092014},
Key = {fds307736}
}
@article{fds307650,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E and Arik, M and Armbruster, AJ},
Title = {Measurement of the production cross section of jets in
association with a Z boson in pp collisions at √s=7 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {7},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP07(2013)032},
Abstract = {Measurements of the production of jets of particles in
association with a Z boson in pp collisions at √s=7 TeV
are presented, using data corresponding to an integrated
luminosity of 4.6 fb-1 collected by the ATLAS experiment at
the Large Hadron Collider. Inclusive and differential jet
cross sections in Z events, with Z decaying into electron or
muon pairs, are measured for jets with transverse momentum p
T > 30 GeV and rapidity |y| < 4.4. The results are compared
to next-to-leading-order perturbative QCD calculations, and
to predictions from different Monte Carlo generators based
on leading-order and next-to-leading-order matrix elements
supplemented by parton showers. [Figure not available: see
fulltext.] © 2013 CERN for the benefit of the ATLAS
collaboration.},
Doi = {10.1007/JHEP07(2013)032},
Key = {fds307650}
}
@article{fds360567,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala,
J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
Title = {Measurement of the production cross section of pairs of
isolated photons in pp collisions at 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)169},
Abstract = {A measurement of prompt photon-pair production in
proton-proton collisions at s = 13 TeV is presented. The
data were recorded by the ATLAS detector at the LHC with an
integrated luminosity of 139 fb−1. Events with two photons
in the well-instrumented region of the detector are
selected. The photons are required to be isolated and have a
transverse momentum of pT,γ1(2)> 40 (30) GeV for the
leading (sub-leading) photon. The differential cross
sections as functions of several observables for the
diphoton system are measured and compared with theoretical
predictions from state-of-the-art Monte Carlo and
fixed-order calculations. The QCD predictions from
next-to-next-to-leading-order calculations and multi-leg
merged calculations are able to describe the measured
integrated and differential cross sections within
uncertainties, whereas lower-order calculations show
significant deviations, demonstrating that higher-order
perturbative QCD corrections are crucial for this process.
The resummed predictions with parton showers additionally
provide an excellent description of the low
transverse-momentum regime of the diphoton system. [Figure
not available: see fulltext.].},
Doi = {10.1007/JHEP11(2021)169},
Key = {fds360567}
}
@article{fds307544,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
M},
Title = {Measurement of the production cross section of prompt J/ψ
mesons in association with a W± boson in pp collisions at
√s = 7 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {4},
Publisher = {Springer Nature},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2014)172},
Abstract = {The process pp → W±J/ψ provides a powerful probe of the
production mechanism of charmonium in hadronic collisions,
and is also sensitive to multiple parton interactions in the
colliding protons. Using the 2011 ATLAS dataset of 4.5 fb-1
of p s = 7TeV pp collisions at the LHC, the first
observation is made of the production of W± + prompt J/
events in hadronic collisions, using W± → μ and J/ψ →
μ+μ-. A yield of 27.4±7.5 -6.5 W± + prompt J/ψ events
is observed, with a statistical significance of 5.1. The
production rate as a ratio to the inclusive W± boson
production rate is measured, and the double parton
scattering contribution to the cross section is estimated.
Copyright CERN, for the benefit of the ATLAS
Collaboration.},
Doi = {10.1007/JHEP04(2014)172},
Key = {fds307544}
}
@article{fds356678,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza,
A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli, M and Antonov,
A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A},
Title = {Measurement of the production cross section of three
isolated photons in pp collisions at √s=8 TeV using the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {781},
Pages = {55-76},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1016/j.physletb.2018.03.057},
Abstract = {A measurement of the production of three isolated photons in
proton–proton collisions at a centre-of-mass energy s=8
TeV is reported. The results are based on an integrated
luminosity of 20.2 fb−1 collected with the ATLAS detector
at the LHC. The differential cross sections are measured as
functions of the transverse energy of each photon, the
difference in azimuthal angle and in pseudorapidity between
pairs of photons, the invariant mass of pairs of photons,
and the invariant mass of the triphoton system. A
measurement of the inclusive fiducial cross section is also
reported. Next-to-leading-order perturbative QCD predictions
are compared to the cross-section measurements. The
predictions underestimate the measurement of the inclusive
fiducial cross section and the differential measurements at
low photon transverse energies and invariant masses. They
provide adequate descriptions of the measurements at high
values of the photon transverse energies, invariant mass of
pairs of photons, and invariant mass of the triphoton
system.},
Doi = {10.1016/j.physletb.2018.03.057},
Key = {fds356678}
}
@article{fds316847,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of the production cross-section of a single top
quark in association with a W boson at 8 TeV with the ATLAS
experiment},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {1},
Pages = {1-48},
Publisher = {Springer Nature},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2016)064},
Abstract = {The cross-section for the production of a single top quark
in association with a W boson in proton-proton collisions at
√s = 8TeV is measured. The dataset corresponds to an
integrated luminosity of 20.3 fb−1, collected by the ATLAS
detector in 2012 at the Large Hadron Collider at CERN.
Events containing two leptons and one central b-jet are
selected. The W t signal is separated from the backgrounds
using boosted decision trees, each of which combines a
number of discriminating variables into one classifier.
Production of W t events is observed with a significance of
7.7σ. The cross-section is extracted in a profile
likelihood fit to the classifier output distributions. The W
t cross-section, inclusive of decay modes, is measured to be
23.0 ± 1.3(stat.)− 3.5+ 3.2(syst.)±1.1(lumi.) pb. The
measured cross-section is used to extract a value for the
CKM matrix element |Vtb| of 1.01 ± 0.10 and a lower limit
of 0.80 at the 95% confidence level. The cross-section for
the production of a top quark and a W boson is also measured
in a fiducial acceptance requiring two leptons with pT> 25
GeV and |η| < 2.5, one jet with pT> 20 GeV and |η| < 2.5,
and ETmiss > 20 GeV, including both W t and top-quark pair
events as signal. The measured value of the fiducial
cross-section is 0.85 ± 0.01(stat.)− 0.07+
0.07(syst.)±0.03(lumi.) pb.},
Doi = {10.1007/JHEP01(2016)064},
Key = {fds316847}
}
@article{fds356683,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the production cross-section of a single top
quark in association with a Z boson in proton–proton
collisions at 13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {780},
Pages = {557-577},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2018.03.023},
Abstract = {The production of a top quark in association with a Z boson
is investigated. The proton–proton collision data
collected by the ATLAS experiment at the LHC in 2015 and
2016 at a centre-of-mass energy of s=13TeV are used,
corresponding to an integrated luminosity of 36.1fb−1.
Events containing three identified leptons (electrons and/or
muons) and two jets, one of which is identified as a b-quark
jet are selected. The major backgrounds are diboson, tt¯
and Z+jets production. A neural network is used to improve
the background rejection and extract the signal. The
resulting significance is 4.2σ in the data and the expected
significance is 5.4σ. The measured cross-section for tZq
production is 600±170(stat.)±140(syst.)fb.},
Doi = {10.1016/j.physletb.2018.03.023},
Key = {fds356683}
}
@article{fds376247,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Bourdarios, CA and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Measurement of the production cross-section of J/ψ and
ψ(2S) mesons in pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {84},
Number = {2},
Year = {2024},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-024-12439-9},
Abstract = {Measurements of the differential production cross-sections
of prompt and non-prompt J/ψ and ψ(2S) mesons with
transverse momenta between 8 and 360 GeV and rapidity in
the range |y|<2 are reported. Furthermore, measurements of
the non-prompt fractions of J/ψ and ψ(2S), and the prompt
and non-prompt ψ(2S)-to-J/ψ production ratios, are
presented. The analysis is performed using 140 fb-1 of
s=13 TeV pp collision data recorded by the ATLAS detector
at the LHC during the years 2015–2018.},
Doi = {10.1140/epjc/s10052-024-12439-9},
Key = {fds376247}
}
@article{fds310381,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
M},
Title = {Measurement of the production of a W boson in association
with a charm quark in pp collisions at √s = 7TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {5},
Pages = {1-67},
Publisher = {Springer-Verlag},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2014)068},
Abstract = {The production of a W boson in association with a single
charm quark is studied using 4.6 fb-1 of pp collision data
at √s = 7TeV collected with the ATLAS detector at the
Large Hadron Collider. In events in which a W boson decays
to an electron or muon, the charm quark is tagged either by
its semileptonic decay to a muon or by the presence of a
charmed meson. The integrated and differential cross
sections as a function of the pseudorapidity of the lepton
from the W-boson decay are measured. Results are compared to
the predictions of next-to-leading-order QCD calculations
obtained from various parton distribution function
parameterisations. The ratio of the strange-to-down
sea-quark distributions is determined to be 0.96+-00.30 at
Q2 = 1.9 GeV, which supports the hypothesis of an
SU(3)-symmetric composition of the light-quark sea.
Additionally the cross-section ratio σ(W+ + c)/σ(W- +c) is
compared to the predictions obtained using parton
distribution function parameterisations with different
assumptions about the s–s quark asymmetry.},
Doi = {10.1007/JHEP05(2014)068},
Key = {fds310381}
}
@article{fds373466,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis,
S and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley,
RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou,
H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai,
G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost, M and Unal, M and Huseynov, N},
Title = {Measurement of the production of a W boson in association
with a charmed hadron in pp collisions at √s=13 TeV with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032012},
Abstract = {The production of a W boson in association with a single
charm quark is studied using 140 fb - 1 of s = 13 TeV
proton-proton collision data collected with the ATLAS
detector at the Large Hadron Collider. The charm quark is
tagged by the presence of a charmed hadron reconstructed
with a secondary-vertex fit. The W boson is reconstructed
from the decay to either an electron or a muon and the
missing transverse momentum present in the event. The
charmed mesons reconstructed are D + → K - π + π + and D
* + → D 0 π + → ( K - π + ) π + and the charge
conjugate decays in the fiducial regions where p T ( e , μ
) > 30 GeV , | η ( e , μ ) | < 2.5 , p T ( D ( * ) ) > 8
GeV , and | η ( D ( * ) ) | < 2.2 . The integrated and
normalized differential cross sections as a function of the
pseudorapidity of the lepton from the W boson decay, and of
the transverse momentum of the charmed hadron, are extracted
from the data using a profile likelihood fit. The measured
total fiducial cross sections are σ fid OS - SS ( W - + D +
) = 50.2 ± 0.2 ( stat ) - 2.3 + 2.4 ( syst ) pb , σ fid OS
- SS ( W + + D - ) = 48.5 ± 0.2 ( stat ) - 2.2 + 2.3 ( syst
) pb , σ fid OS - SS ( W - + D * + ) = 51.1 ± 0.4 ( stat )
- 1.8 + 1.9 ( syst ) pb , and σ fid OS - SS ( W + + D * - )
= 50.0 ± 0.4 ( stat ) - 1.8 + 1.9 ( syst ) pb . Results are
compared with the predictions of next-to-leading-order
quantum chromodynamics calculations performed using
state-of-the-art parton distribution functions.
Additionally, the ratio of charm to anticharm production
cross sections is studied to probe the s - s ¯ quark
asymmetry. The ratio is found to be R c ± = 0.971 ± 0.006
( stat ) ± 0.011 ( syst ) . The ratio and cross-section
measurements are consistent with the predictions obtained
with parton distribution function sets that have a symmetric
s - s ¯ sea, indicating that any s - s ¯ asymmetry in the
Bjorken- x region relevant for this measurement is
small.},
Doi = {10.1103/PhysRevD.108.032012},
Key = {fds373466}
}
@article{fds307768,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
R and Ask, S},
Title = {Measurement of the pseudorapidity and transverse momentum
dependence of the elliptic flow of charged particles in
lead-lead collisions at sNN=2.76 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {707},
Number = {3-4},
Pages = {330-348},
Publisher = {Elsevier BV},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2011.12.056},
Abstract = {This Letter describes the measurement of elliptic flow of
charged particles in lead-lead collisions at sNN=2.76 TeV
using the ATLAS detector at the Large Hadron Collider (LHC).
The results are based on an integrated luminosity of
approximately 7 μb-1. Elliptic flow is measured over a wide
region in pseudorapidity, |η|<2.5, and over a broad range
in transverse momentum, 0.5<pT<20 GeV. The elliptic flow
parameter v2 is obtained by correlating individual tracks
with the event plane measured using energy deposited in the
forward calorimeters. As a function of transverse momentum,
v2(pT) reaches a maximum at pT of about 3 GeV, then
decreases and becomes weakly dependent on pT above 7-8 GeV.
Over the measured pseudorapidity region, v2 is found to be
only weakly dependent on η, with less variation than
observed at lower beam energies. The results are discussed
in the context of previous measurements at lower collision
energies, as well as recent results from the LHC. © 2011
CERN.},
Doi = {10.1016/j.physletb.2011.12.056},
Key = {fds307768}
}
@article{fds308000,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
MA},
Title = {Measurement of the ratio of branching fractions B(B±→J/
ψπ±)/B(B±→J/ψK±)},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112003},
Abstract = {We report a measurement of the ratio of branching fractions
of the decays B±→J/ψπ± and B±→J/ψK± using the CDF
II detector at the Fermilab Tevatron Collider. The signal
from the Cabbibo-suppressed B±→J/ψπ± decay is
separated from B±→J/ψK± using the B±→J/ψK±
invariant mass distribution and the kinematical differences
of the hadron track in the two decay modes. From a sample of
220pb-1 of pp̄ collisions at s=1.96TeV, we observe 91±15
B±→J/ψπ± events together with 1883±34 B±→J/ψK±
events. The ratio of branching fractions is found to be
B(B±→J/ψπ±)/ B(B±→J/ψK±)=(4.86±0.82(stat)±0.15(syst))%.
© 2009 The American Physical Society.},
Doi = {10.1103/PhysRevD.79.112003},
Key = {fds308000}
}
@article{fds308122,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo,
T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
I and Gallinaro, M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris,
N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare,
M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser,
J and Hays, C and Heijboer, A and Heinemann, B and Heinrich, J and Herndon,
M and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato,
Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian,
C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh,
YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin,
J},
Title = {Measurement of the ratio of branching fractions
B(D0→K+π-)/ B(D0→K-π+) using the CDF II
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {74},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.031109},
Abstract = {We present a measurement of RB, the ratio of the branching
fraction for the rare decay D0→K+π- to that for the
Cabibbo-favored decay D0→K-π+. Charge-conjugate decays
are implicitly included. A signal of 2005±104 events for
the decay D0→K+π- is obtained using the CDF II detector
at the Fermilab Tevatron collider. The data set corresponds
to an integrated luminosity of 0.35fb-1 produced in p̄p
collisions at s=1.96TeV. Assuming no mixing, we find
RB=[4.05±0.21(stat)±0.11(syst)] ×10-3. This measurement
is consistent with the world average, and comparable in
accuracy with the best measurements from other experiments.
© 2006 The American Physical Society.},
Doi = {10.1103/PhysRevD.74.031109},
Key = {fds308122}
}
@article{fds356613,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger,
M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou,
C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Arduh, FA and Arguin, JF},
Title = {Measurement of the ratio of cross sections for inclusive
isolated-photon production in pp collisions at √s = 13 and
8 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {4},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2019)093},
Abstract = {The ratio of the cross sections for inclusive
isolated-photon production in pp collisions at
centre-of-mass energies of 13 and 8 TeV is measured using
the ATLAS detector at the LHC. The integrated luminosities
of the 13 TeV and 8 TeV datasets are 3.2 fb −1 and 20.2 fb
−1 , respectively. The ratio is measured as a function of
the photon transverse energy in different regions of the
photon pseudorapidity. The predictions from
next-to-leading-order perturbative QCD calculations are
compared with the measured ratio. The experimental
systematic uncertainties as well as the uncertainties
affecting the predictions are evaluated taking into account
the correlations between the two centre-of-mass energies,
resulting in a reduction of up to a factor of 2.5 (5) in the
experimental (theoretical) systematic uncertainties. The
predictions based on several parameterisations of the proton
parton distribution functions agree with the data within the
reduced experimental and theoretical uncertainties. In
addition, this ratio to that of the fiducial cross sections
for Z boson production at 13 and 8 TeV using the decay
channels Z → e + e − and Z → μ + μ − is made and
compared with the theoretical predictions. In this double
ratio, a further reduction of the experimental uncertainty
is obtained because the uncertainties arising from the
luminosity measurement cancel out. The predictions describe
the measurements of the double ratio within the theoretical
and experimental uncertainties.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP04(2019)093},
Key = {fds356613}
}
@article{fds308184,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette,
F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR},
Title = {Measurement of the ratio of differential cross sections for
W and Z boson production as a function of transverse
momentum in pp̄ collisions at √s = 1.8
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {517},
Number = {3-4},
Pages = {299-308},
Publisher = {Elsevier BV},
Year = {2001},
Month = {October},
url = {http://dx.doi.org/10.1016/S0370-2693(01)01020-6},
Abstract = {We report on a measurement of the ratio of the differential
cross sections for W and Z boson production as a function of
transverse momentum in proton-antiproton collisions at √s
= 1.8 TeV. This measurement uses data recorded by the DØ
detector at the Fermilab Tevatron in 1994-1995. It
represents the first investigation of a proposal that ratios
between W and Z observables can be calculated reliably using
perturbative QCD, even when the individual observables are
not. Using the ratio of differential cross sections reduces
both experimental and theoretical uncertainties, and can
therefore provide smaller overall uncertainties in the
measured mass and width of the W boson than current methods
used at hadron colliders. © 2001 Elsevier Science B.V. All
rights reserved.},
Doi = {10.1016/S0370-2693(01)01020-6},
Key = {fds308184}
}
@article{fds308081,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Cyr, D and Daronco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart,
D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza,
BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher,
R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster,
GW and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay,
C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson,
A and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths,
M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic, V and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Sjolin, J and Slaughter,
AJ},
Title = {Measurement of the ratios of branching fractions B(Bs0→Ds-
π+π+π-)/B(B0→D-π+π+π-) and B(Bs0→Ds-π+)/
B(B0→D-π+)},
Journal = {Physical Review Letters},
Volume = {98},
Number = {6},
Pages = {061802},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevLett.98.061802},
Abstract = {Using 355pb-1 of data collected by the CDF II detector in
pp̄ collisions at s=1.96TeV at the Fermilab Tevatron, we
study the fully reconstructed hadronic decays
B(s)0→D(s)-π+ and B(s)0→D(s)- π+π+π-. We present the
first measurement of the ratio of branching fractions
B(Bs0→Ds-π+π+π-)/B(B0→D-π+π+π-)=1.
05±0.10(stat)±0.22(syst). We also update our measurement
of B(Bs0→Ds-π+)/B(B0→D-π+) to 1.13±0.08(stat)±0.
23(syst), improving the statistical uncertainty by more than
a factor of 2. We find B(Bs0→Ds-π+)=[3.8±0.3(stat)±1.3(syst)]×10-3
and B(Bs0→Ds-π+π+π-)=[8.4±0.8(stat)±3.2(syst)]
×10-3. © 2007 The American Physical Society.},
Doi = {10.1103/PhysRevLett.98.061802},
Key = {fds308081}
}
@article{fds361223,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, J and DiTuro, P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Sciverez, MG and Garfinkel, AF and Gay,
C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Costa, JGD and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper,
S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer, A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel, M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute,
M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman,
R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov,
AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori,
L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli,
S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez,
C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro,
A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro,
MD},
Title = {Measurement of the ratios of branching fractions
B(Bs0→Ds-π+)/ B(B0→D-π+) and B(B+→D̄0π+)/B(B0→D-π+)},
Journal = {Physical Review Letters},
Volume = {96},
Number = {19},
Pages = {191801},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevLett.96.191801},
Abstract = {We report an observation of the decay Bs0→Ds-π+ in pp̄
collisions at s=1.96TeV using 115pb-1 of data collected by
the CDF II detector at the Fermilab Tevatron. We observe
83±11(stat) Bs0→Ds-π+ candidates, representing a large
increase in statistics over previous measurements and the
first observation of this decay at a pp̄ collider. We
present the first measurement of the relative branching
fraction B(Bs0→Ds-π+)/B(B0→D-π+)=1.32±0.18(stat)±0.38(syst)
. We also measure B(B+→D̄0π+)/B(B0→D-π+)=1.97±0.
10(stat)±0.21(syst), which is consistent with previous
measurements. © 2006 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.96.191801},
Key = {fds361223}
}
@article{fds321127,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Measurement of the relative width difference of the
B0‐ B¯ 0 system with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {6},
Publisher = {Springer Nature},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2016)081},
Abstract = {Abstract: This paper presents the measurement of the
relative width difference ΔΓd/Γd of the B0‐ B¯ 0
system using the data collected by the ATLAS experiment at
the LHC in pp collisions at s=7 TeV and s=8 TeV and
corresponding to an integrated luminosity of 25.2 fb−1.
The value of ΔΓd/Γd is obtained by comparing the
decay-time distributions of B0 → J/ψKS and B0 →
J/ψK*0(892) decays. The result is ΔΓd/Γd = (−0.1±1.1
(stat.)± 0.9 (syst.)) × 10−2. Currently, this is the
most precise single measurement of ΔΓd/Γd. It agrees with
the Standard Model prediction and the measurements by other
experiments.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP06(2016)081},
Key = {fds321127}
}
@article{fds373906,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena,
E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster,
AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio,
S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos,
G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry,
T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans,
G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura,
P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet,
D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A},
Title = {Measurement of the Sensitivity of Two-Particle Correlations
in pp Collisions to the Presence of Hard
Scatterings.},
Journal = {Physical review letters},
Volume = {131},
Number = {16},
Pages = {162301},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.162301},
Abstract = {A key open question in the study of multiparticle production
in high-energy pp collisions is the relationship between the
"ridge"-i.e., the observed azimuthal correlations between
particles in the underlying event that extend over all
rapidities-and hard or semihard scattering processes. In
particular, it is not known whether jets or their soft
fragments are correlated with particles in the underlying
event. To address this question, two-particle correlations
are measured in pp collisions at sqrt[s]=13 TeV using
data collected by the ATLAS experiment at the LHC, with an
integrated luminosity of 15.8 pb^{-1}, in two different
configurations. In the first case, charged particles
associated with jets are excluded from the correlation
analysis, while in the second case, correlations are
measured between particles within jets and charged particles
from the underlying event. Second-order flow coefficients,
v_{2}, are presented as a function of event multiplicity and
transverse momentum. These measurements show that excluding
particles associated with jets does not affect the measured
correlations. Moreover, particles associated with jets do
not exhibit any significant azimuthal correlations with the
underlying event, ruling out hard processes contributing to
the ridge.},
Doi = {10.1103/physrevlett.131.162301},
Key = {fds373906}
}
@booklet{Abbott98h,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Measurement of the shape of the transverse momentum
distribution of W bosons produced in pp¯ collisions at √s
= 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {80},
Number = {25},
Pages = {5498-5503},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.5498},
Abstract = {The shape of the transverse momentum distribution of W
bosons (pWT) produced in pp¯ collisions at √s = 1.8 TeV
is measured with the D0 detector at Fermilab. The result is
compared with QCD perturbative and resummation calculations
over the pWT range from 0 to 200 GeV/c. The shape of the
distribution is consistent with the theoretical prediction.
© 1998 The American Physical Society.},
Doi = {10.1103/PhysRevLett.80.5498},
Key = {Abbott98h}
}
@article{fds347514,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of the single top quark production cross section
and},
Journal = {Physical Review D},
Volume = {93},
Number = {3},
Year = {2016},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.93.032011},
Abstract = {An updated measurement of the single top quark production
cross section is presented using the full data set collected
by the Collider Detector at Fermilab (CDF), corresponding to
9.5 fb-1 of integrated luminosity from proton-antiproton
collisions at 1.96 TeV center-of-mass energy. The events
selected contain an imbalance in the total transverse
momentum, jets identified as containing b quarks, and no
identified leptons. The sum of the s- and t-channel single
top quark cross sections is measured to be 3.53-1.16+1.25 pb
and a lower limit on the magnitude of the top-to-bottom
quark coupling, |Vtb| of 0.63, is obtained at the 95%
credibility level. These measurements are combined with
previously reported CDF results obtained from events with an
imbalance in total transverse momentum, jets identified as
originating from b quarks, and one identified lepton. The
combined cross section is measured to be 3.02-0.48+0.49 pb
and a lower limit on |Vtb| of 0.84 is obtained at the 95%
credibility level.},
Doi = {10.1103/PhysRevD.93.032011},
Key = {fds347514}
}
@article{fds313620,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn,
SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hirschbuehl, D and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Measurement of the single top quark production cross section
and |Vtb| in events with one charged lepton, large missing
transverse energy, and jets at CDF.},
Journal = {Physical review letters},
Volume = {113},
Number = {26},
Pages = {261804},
Year = {2014},
Month = {December},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.113.261804},
Abstract = {We report a measurement of single top quark production in
proton-antiproton collisions at a center-of-mass energy of
sqrt[s]=1.96 TeV using a data set corresponding to
7.5 fb(-1) of integrated luminosity collected by the
Collider Detector at Fermilab. We select events consistent
with the single top quark decay process t→Wb→ℓνb by
requiring the presence of an electron or muon, a large
imbalance of transverse momentum indicating the presence of
a neutrino, and two or three jets including at least one
originating from a bottom quark. An artificial neural
network is used to discriminate the signal from backgrounds.
We measure a single top quark production cross section of
3.04(-0.53)(+0.57) pb and set a lower limit on the
magnitude of the coupling between the top quark and bottom
quark |Vtb|>0.78 at the 95% credibility level.},
Doi = {10.1103/physrevlett.113.261804},
Key = {fds313620}
}
@article{fds308003,
Author = {Aaltonen, T and others},
Title = {Measurement of the Single-Top-Quark Production Cross Section
at CDF},
Journal = {Physical Review Letters},
Volume = {101},
Number = {25},
Pages = {252001},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.252001},
Abstract = {We report a measurement of the single-top-quark production
cross section in 2.2 fb-1 of pp̅ collision data
collected by the Collider Detector at Fermilab at
sqrt[s]=1.96 TeV. Candidate events are classified as
signal-like by three parallel analyses which use likelihood,
matrix element, and neural network discriminants. These
results are combined in order to improve the sensitivity. We
observe a signal consistent with the standard model
prediction, but inconsistent with the background-only model
by 3.7 standard deviations with a median expected
sensitivity of 4.9 standard deviations. We measure a cross
section of 2.2-0.6+0.7(stat+syst) pb, extract the
Cabibbo-Kobayashi-Maskawa matrix-element value
|Vtb|=0.88-0.12+0.13(stat+syst) ± 0.07(theory), and
set the limit |Vtb|>0.66 at the 95% C.L.},
Doi = {10.1103/physrevlett.101.252001},
Key = {fds308003}
}
@article{fds347459,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
J},
Title = {Measurement of the Soft-Drop Jet Mass in pp Collisions at
sqrt[s]=13 TeV with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {121},
Number = {9},
Pages = {092001},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.121.092001},
Abstract = {Jet substructure observables have significantly extended the
search program for physics beyond the standard model at the
Large Hadron Collider. The state-of-the-art tools have been
motivated by theoretical calculations, but there has never
been a direct comparison between data and calculations of
jet substructure observables that are accurate beyond
leading-logarithm approximation. Such observables are
significant not only for probing the collinear regime of QCD
that is largely unexplored at a hadron collider, but also
for improving the understanding of jet substructure
properties that are used in many studies at the Large Hadron
Collider. This Letter documents a measurement of the first
jet substructure quantity at a hadron collider to be
calculated at next-to-next-to-leading-logarithm accuracy.
The normalized, differential cross section is measured as a
function of log_{10}ρ^{2}, where ρ is the ratio of the
soft-drop mass to the ungroomed jet transverse momentum.
This quantity is measured in dijet events from
32.9 fb^{-1} of sqrt[s]=13 TeV proton-proton
collisions recorded by the ATLAS detector. The data are
unfolded to correct for detector effects and compared to
precise QCD calculations and leading-logarithm
particle-level Monte Carlo simulations.},
Doi = {10.1103/physrevlett.121.092001},
Key = {fds347459}
}
@article{fds356651,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A},
Title = {Measurement of the suppression and azimuthal anisotropy of
muons from heavy-flavor decays in Pb+Pb collisions at sNN
=2.76 TeV with the ATLAS detector},
Journal = {Physical Review C},
Volume = {98},
Number = {4},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevC.98.044905},
Abstract = {ATLAS measurements of the production of muons from
heavy-flavor decays in sNN=2.76 TeV Pb+Pb collisions and
s=2.76 TeV pp collisions at the LHC are presented.
Integrated luminosities of 0.14 nb-1 and 570 nb-1 are used
for the Pb+Pb and pp measurements, respectively, which are
performed over the muon transverse momentum range 4<pT<14
GeV and for five Pb+Pb centrality intervals. Backgrounds
arising from in-flight pion and kaon decays, hadronic
showers, and misreconstructed muons are statistically
removed using a template-fitting procedure. The heavy-flavor
muon differential cross sections and per-event yields are
measured in pp and Pb+Pb collisions, respectively. The
nuclear modification factor RAA obtained from these is
observed to be independent of pT, within uncertainties, and
to be less than unity, which indicates suppressed production
of heavy-flavor muons in Pb+Pb collisions. For the 10% most
central Pb+Pb events, the measured RAA is approximately
0.35. The azimuthal modulation of the heavy-flavor muon
yields is also measured and the associated Fourier
coefficients vn for n=2, 3, and 4 are given as a function of
pT and centrality. They vary slowly with pT and show a
systematic variation with centrality which is characteristic
of other anisotropy measurements, such as that observed for
inclusive hadrons. The measured RAA and vn values are also
compared with theoretical calculations.},
Doi = {10.1103/PhysRevC.98.044905},
Key = {fds356651}
}
@article{fds308128,
Author = {Abulencia, and A, and others},
Title = {Measurement of the t anti-t production cross section in
$p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV in the all
hadronic decay mode},
Journal = {Phys. Rev.},
Volume = {D74},
Number = {7},
Pages = {072005},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.072005},
Abstract = {We report a measurement of the tt-bar production cross
section using the CDF II detector at the Fermilab Tevatron.
The analysis is performed using 322 pb-1 of p anti-p
collisions at s**(1/2) = 1.96 TeV. The data consist of
events selected with six or more hadronic jets with
additional kinematic requirements. At least one of these
jets must be identified as a b-quark jet by the
reconstruction of a secondary vertex. The cross section is
measured to be sigma_tt-bar = 7.5 +/- 2.1(stat.)+3.3_-2.2(syst.)+0.5_-0.4(lumi.)
pb, which is consistent with the standard model
prediction.},
Doi = {10.1103/PhysRevD.74.072005},
Key = {fds308128}
}
@article{fds308120,
Author = {Acosta, and D, and others},
Title = {Measurement of the t anti-t production cross section in p
anti-p collisions at sqrt[s]=1.96 TeV using lepton + jets
events with secondary vertex b-tagging},
Journal = {Phys. Rev.},
Volume = {D71},
Number = {7},
Pages = {052003},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.74.072006},
Abstract = {http://arxiv.org/abs/hep-ex/0410041},
Doi = {10.1103/PhysRevD.74.072006},
Key = {fds308120}
}
@article{fds356755,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik,
M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of the t t production cross section in the
τ+jets final state in pp collisions at s =8 TeV using the
ATLAS detector},
Journal = {Physical Review D},
Volume = {95},
Number = {7},
Year = {2017},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.95.072003},
Abstract = {A measurement of the inclusive pp→tt+X production cross
section in the τ+jets final state using only the hadronic
decays of the τ lepton is presented. The measurement is
performed using 20.2 fb-1 of proton-proton collision data
recorded at a center-of-mass energy of s=8 TeV with the
ATLAS detector at the Large Hadron Collider. The cross
section is measured via a counting experiment by imposing a
set of selection criteria on the identification and
kinematic variables of the reconstructed particles and jets,
and on event kinematic variables and characteristics. The
production cross section is measured to be σtt=239±29 pb,
which is in agreement with the measurements in other final
states and the theoretical predictions at this
center-of-mass energy.},
Doi = {10.1103/PhysRevD.95.072003},
Key = {fds356755}
}
@article{fds359997,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
Title = {Measurement of the t t¯ t t¯ production cross section in
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)118},
Abstract = {A measurement of four-top-quark production using
proton-proton collision data at a centre-of-mass energy of
13 TeV collected by the ATLAS detector at the Large Hadron
Collider corresponding to an integrated luminosity of 139
fb−1 is presented. Events are selected if they contain a
single lepton (electron or muon) or an opposite-sign lepton
pair, in association with multiple jets. The events are
categorised according to the number of jets and how likely
these are to contain b-hadrons. A multivariate technique is
then used to discriminate between signal and background
events. The measured four-top-quark production cross section
is found to be 26−15+17 fb, with a corresponding observed
(expected) significance of 1.9 (1.0) standard deviations
over the background-only hypothesis. The result is combined
with the previous measurement performed by the ATLAS
Collaboration in the multilepton final state. The combined
four-top-quark production cross section is measured to be
24−6+7 fb, with a corresponding observed (expected) signal
significance of 4.7 (2.6) standard deviations over the
background-only predictions. It is consistent within 2.0
standard deviations with the Standard Model expectation of
12.0 ± 2.4 fb. [Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP11(2021)118},
Key = {fds359997}
}
@article{fds307777,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Measurement of the t-channel single top-quark production
cross section in pp collisions at s=7 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {717},
Number = {4-5},
Pages = {330-350},
Publisher = {Elsevier BV},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2012.09.031},
Abstract = {We report a measurement of the cross section of single
top-quark production in the t-channel using 1.04 fb−1 of
pp collision data at s=7 TeV recorded with the ATLAS
detector at the LHC. Selected events feature one electron or
muon, missing transverse momentum, and two or three jets,
exactly one of them identified as originating from a b
quark. The cross section is measured by fitting the
distribution of a multivariate discriminant constructed with
a neural network, yielding σt=83±4(stat.)−19+20(syst.)
pb, which is in good agreement with the prediction of the
Standard Model. Using the ratio of the measured to the
theoretically predicted cross section and assuming that the
top-quark-related CKM matrix elements obey the relation
|Vtb|≫|Vts|,|Vtd|, the coupling strength at the W-t-b
vertex is determined to be |Vtb|=1.13−0.13+0.14. If it is
assumed that |Vtb|⩽1 a lower limit of |Vtb|>0.75 is
obtained at the 95% confidence level.},
Doi = {10.1016/j.physletb.2012.09.031},
Key = {fds307777}
}
@article{fds310279,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of the top pair production cross section in 8
TeV proton-proton collisions using kinematic information in
the lepton + jets final state with ATLAS},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.91.112013},
Abstract = {A measurement is presented of the (formula presented)
inclusive production cross section in pp collisions at a
center-of-mass energy of (formula presented) using data
collected by the ATLAS detector at the CERN Large Hadron
pffiffi Collider. The measurement was performed in the
lepton + jets final state using a data set corresponding to
an integrated luminosity of 20.3 fb-1. The cross section was
obtained using a likelihood discriminant fit and b-jet
identification was used to improve the signal-to-background
ratio. The inclusive tt production cross section was
measured to be (formula presented) pb assuming a top-quark
mass of 172.5 GeV, in good agreement with the theoretical
prediction of (formula presented) pb. The (formula
presented) production cross section in the fiducial region
determined by the detector acceptance is also
reported.},
Doi = {10.1103/PhysRevD.91.112013},
Key = {fds310279}
}
@article{fds307881,
Author = {Aaltonen, and T, and al, E},
Title = {Measurement of the top pair production cross section in the
$\mathrm{{lepton}}+\mathrm{{jets}}$ channel using a jet
flavor discriminant},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {3},
Pages = {031101},
Publisher = {American Physical Society},
Year = {2011},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.84.031101},
Abstract = {We present a new method to measure the top quark pair
production cross section and the background rates with data
corresponding to an integrated luminosity of 2.7fb-1 from
pp̄ collisions at √s=1.96TeV collected with the CDF II
Detector. We select events with a single electron or muon
candidate, missing transverse energy, and at least one
b-tagged jet. We perform a simultaneous fit to a jet flavor
discriminant across nine samples defined by the number of
jets and b tags. An advantage of this approach is that many
systematic uncertainties are measured in situ and inversely
scale with integrated luminosity. We measure a top cross
section of σ tt̄=7.64±0.57(stat+syst)±0.45(luminosity)pb.
© 2011 American Physical Society.},
Doi = {10.1103/PhysRevD.84.031101},
Key = {fds307881}
}
@article{fds307931,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the top pair production cross section in the
dilepton decay channel in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
collisions at $\sqrt{s}=1.96\,\,TeV$},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {5},
Pages = {052002},
Publisher = {American Physical Society},
Year = {2010},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.82.052002},
Abstract = {A measurement of the tt̄ production cross section in pp̄
collisions at √s=1.96TeV using events with two leptons,
missing transverse energy, and jets is reported. The data
were collected with the CDF II detector. The result in a
data sample corresponding to an integrated luminosity
2.8fb-1 is σtt̄=6.27±0.73(stat) ±0.63(syst)±0.39(lum)pb.
for an assumed top mass of 175GeV/c2. © 2010 The American
Physical Society.},
Doi = {10.1103/PhysRevD.82.052002},
Key = {fds307931}
}
@article{fds307565,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson,
TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand,
S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Measurement of the top quark charge in pp collisions at √s
= 7 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {11},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP11(2013)031},
Abstract = {A measurement of the top quark electric charge is carried
out in the ATLAS experiment at the Large Hadron Collider
using 2.05 fb-1 of data at a centre-of-mass energy of 7TeV.
In units of the elementary electric charge, the top quark
charge is determined to be 0.64 ± 0.02 (stat.) ± 0.08
(syst.) from the charges of the top quark decay products in
single lepton tt̄ candidate events. This excludes models
that propose a heavy quark of electric charge -4/3, instead
of the Standard Model top quark, with a significance of more
than 8σ. Copyright CERN.},
Doi = {10.1007/JHEP11(2013)031},
Key = {fds307565}
}
@article{fds307603,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Measurement of the top quark forward-backward production
asymmetry and its dependence on event kinematic
properties},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.87.092002},
Abstract = {We present new measurements of the inclusive
forward-backward tt̄ production asymmetry, AFB, and its
dependence on several properties of the tt̄ system. The
measurements are performed with the full Tevatron data set
recorded with the CDF II detector during pp̄ collisions at
√s=1.96 TeV, corresponding to an integrated luminosity of
9.4 fb -1. We measure the asymmetry using the rapidity
difference Δy=yt-yt̄. Parton-level results are derived,
yielding an inclusive asymmetry of 0.164±0.047(stat+syst).
We establish an approximately linear dependence of AFB on
the top-quark pair mass Mtt̄ and the rapidity difference
|Δy| at detector and parton levels. Assuming the standard
model, the probabilities to observe the measured values or
larger for the detector-level dependencies are 7.4×10-3 and
2.2×10-3 for Mtt̄ and |Δy| respectively. Lastly, we study
the dependence of the asymmetry on the transverse momentum
of the tt̄ system at the detector level. These results are
consistent with previous lower-precision measurements and
provide additional quantification of the functional
dependencies of the asymmetry. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.87.092002},
Key = {fds307603}
}
@article{fds307922,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the Top Quark Mass and $p \bar{p} \to t
\bar{t}$ Cross Section in the All-Hadronic Mode with the
CDFII Detector},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {5},
Pages = {052011},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.052011},
Abstract = {http://arxiv.org/abs/1002.0365},
Doi = {10.1103/PhysRevD.81.052011},
Key = {fds307922}
}
@article{fds307984,
Author = {Aaltonen, T and others},
Title = {Measurement of the top quark mass at CDF using the
``neutrino phi weighting'' template method on a lepton plus
isolated track sample},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {7},
Pages = {072005},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.072005},
Abstract = {We present a measurement of the top quark mass with tt̄
dilepton events produced in pp̄ collisions at the Fermilab
Tevatron (s=1.96TeV) and collected by the CDF II detector. A
sample of 328 events with a charged electron or muon and an
isolated track, corresponding to an integrated luminosity of
2.9fb-1, are selected as tt̄ candidates. To account for the
unconstrained event kinematics, we scan over the phase space
of the azimuthal angles (ν1,ν2) of neutrinos and
reconstruct the top quark mass for each ν1, ν2 pair by
minimizing a χ2 function in the tt̄ dilepton hypothesis.
We assign χ2-dependent weights to the solutions in order to
build a preferred mass for each event. Preferred mass
distributions (templates) are built from simulated tt̄ and
background events, and parametrized in order to provide
continuous probability density functions. A likelihood fit
to the mass distribution in data as a weighted sum of signal
and background probability density functions gives a top
quark mass of 165.5-3.3+3.4(stat)±3. 1(syst)GeV/c2. © 2009
The American Physical Society.},
Doi = {10.1103/PhysRevD.79.072005},
Key = {fds307984}
}
@article{fds308070,
Author = {Abulencia, and A, and others},
Title = {Measurement of the Top Quark Mass in $p\bar{p}$Collisions at
$\sqrt{s} = 1.96$ TeV using the Decay Length
Technique},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {7},
Pages = {071102},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.071102},
Abstract = {We report the first measurement of the top quark mass using
the decay length technique in p[overline p] collisions at a
center-of-mass energy of 1.96 TeV. This technique uses the
measured flight distance of the b hadron to infer the mass
of the top quark in lepton plus jets events with missing
transverse energy. It relies solely on tracking and avoids
the jet energy scale uncertainty that is common to all other
methods used so far. We apply our novel method to a 695 pb-1
data sample recorded by the CDF II detector at Fermilab and
extract a measurement of mt=180.7-13.4+15.5(stat.)$\pm$8.6(syst.)
GeV/c2. While the uncertainty of this result is larger than
that of other measurements, the dominant uncertainties in
the decay length technique are uncorrelated with those in
other methods. This result can help reduce the overall
uncertainty when combined with other existing measurements
of the top quark mass.},
Doi = {10.1103/PhysRevD.75.071102},
Key = {fds308070}
}
@article{fds307822,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M},
Title = {Measurement of the top quark mass in the all-hadronic mode
at CDF},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {714},
Number = {1},
Pages = {24-31},
Publisher = {Elsevier BV},
Year = {2012},
Month = {July},
url = {http://dx.doi.org/10.1016/j.physletb.2012.06.007},
Abstract = {A measurement of the top quark mass (M top) in the
all-hadronic decay channel is presented. It uses 5.8 fb -1
of pp data collected with the CDF II detector at the
Fermilab Tevatron Collider. Events with six to eight jets
are selected by a neural network algorithm and by the
requirement that at least one of the jets is tagged as a
b-quark jet. The measurement is performed with a likelihood
fit technique, which simultaneously determines M top and the
jet energy scale (JES) calibration. The fit yields a value
of M top=172.5±1.4(stat)±1.0(JES)±1.1(syst) GeV/c 2. ©
2012 Elsevier B.V.},
Doi = {10.1016/j.physletb.2012.06.007},
Key = {fds307822}
}
@article{fds308213,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G},
Title = {Measurement of the top quark mass in the dilepton
channel},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {5},
Pages = {1-21},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.60.052001},
Abstract = {We report a measurement of the top quark mass using six
candidate events for the process (Formula presented),
observed in the D0 experiment at the Fermilab (Formula
presented) collider. Using maximum likelihood fits to the
dynamics of the decays, we measure a mass for the top quark
of (Formula presented). We combine this result with our
previous measurement in the (Formula presented) channel to
obtain (Formula presented) as the best value of the mass of
the top quark measured by D0. © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevD.60.052001},
Key = {fds308213}
}
@article{fds307885,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
Title = {Measurement of the top quark mass in the lepton+jets channel
using the lepton transverse momentum},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {698},
Number = {5},
Pages = {371-379},
Publisher = {Elsevier BV},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2011.03.041},
Abstract = {This Letter reports a measurement of the top quark mass,
Mtop, in data from pp- collisions at s=1.96 TeV
corresponding to 2.7 fb-1 of integrated luminosity at the
Fermilab Tevatron using the CDF II detector. Events with the
lepton+jets topology are selected. An unbinned likelihood is
constructed based on the dependence of the lepton transverse
momentum, PT, on Mtop. A maximum likelihood fit to the data
yields a measured mass Mtop=176.9±8.0stat±2.7syst GeV/c2.
In this measurement, the contribution by the jet energy
scale uncertainty to the systematic error is negligible. The
result provides an important consistency test for other Mtop
measurements where explicit use of the jet energy is made
for deriving the top quark mass. © 2011 Elsevier
B.V.},
Doi = {10.1016/j.physletb.2011.03.041},
Key = {fds307885}
}
@article{fds356610,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella, L and Arabidze, G and Araque,
JP and Araujo Ferraz, V and Araujo Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ},
Title = {Measurement of the top quark mass in the tt¯ →
lepton+jets channel from √s=8 TeV ATLAS data and
combination with previous results},
Journal = {European Physical Journal C},
Volume = {79},
Number = {4},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6757-9},
Abstract = {The top quark mass is measured using a template method in
the tt¯ → lepton + jets channel (lepton is e or μ) using
ATLAS data recorded in 2012 at the LHC. The data were taken
at a proton–proton centre-of-mass energy of s=8 TeV and
correspond to an integrated luminosity of 20.2 fb - 1 . The
tt¯ → lepton + jets channel is characterized by the
presence of a charged lepton, a neutrino and four jets, two
of which originate from bottom quarks (b). Exploiting a
three-dimensional template technique, the top quark mass is
determined together with a global jet energy scale factor
and a relative b-to-light-jet energy scale factor. The mass
of the top quark is measured to be mtop=172.08±0.39(stat)±0.82(syst) GeV.
A combination with previous ATLAS m top measurements gives
mtop=172.69±0.25(stat)±0.41(syst) GeV.},
Doi = {10.1140/epjc/s10052-019-6757-9},
Key = {fds356610}
}
@article{fds321133,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of the top quark mass in the tt¯→dilepton
channel from √s=8 TeV ATLAS data},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {761},
Pages = {350-371},
Publisher = {Elsevier BV},
Year = {2016},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.042},
Abstract = {The top quark mass is measured in the tt¯→dilepton
channel (lepton=e,μ) using ATLAS data recorded in the year
2012 at the LHC. The data were taken at a proton–proton
centre-of-mass energy of s=8 TeV and correspond to an
integrated luminosity of about 20.2 fb−1. Exploiting the
template method, and using the distribution of invariant
masses of lepton–b-jet pairs, the top quark mass is
measured to be mtop=172.99±0.41 (stat)±0.74 (syst) GeV,
with a total uncertainty of 0.84 GeV. Finally, a combination
with previous ATLAS mtop measurements from s=7 TeV data in
the tt¯→dilepton and tt¯→lepton+jets channels results
in mtop=172.84±0.34 (stat)±0.61 (syst) GeV, with a total
uncertainty of 0.70 GeV.},
Doi = {10.1016/j.physletb.2016.08.042},
Key = {fds321133}
}
@article{fds310333,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
Title = {Measurement of the top quark mass in the [Formula: see text]
and [Formula: see text] channels using [Formula: see
text] [Formula: see text] ATLAS data.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {330},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3544-0},
Doi = {10.1140/epjc/s10052-015-3544-0},
Key = {fds310333}
}
@booklet{Abbott98m,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros, Y and Dudko,
LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga, MK and Featherly,
J and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk,
HE},
Title = {Measurement of the top quark mass using dilepton
events},
Journal = {Physical Review Letters},
Volume = {80},
Number = {10},
Pages = {2063-2068},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.2063},
Abstract = {The D0 Collaboration has performed a measurement of the top
quark mass mt based on six candidate events for the process
tt- → bW+bW-, where the W bosons decay to eν or μν.
This sample was collected during an exposure of the D0
detector to an integrated luminosity of 125pb-1 of √ s =
1.8 TeV pp collisions. We obtain mt = 168.4 ± 12.3(stat) ±
3.6(syst) GeV/c2, consistent with the measurement obtained
using single-lepton events. Combination of the single-lepton
and dilepton results yields mt = 172.0 ± 7.5 GeV/c2. ©
1998 The American Physical Society.},
Doi = {10.1103/PhysRevLett.80.2063},
Key = {Abbott98m}
}
@article{fds308124,
Author = {Abulencia, and A, and others},
Title = {Measurement of the top quark mass using template methods on
dilepton events in proton antiproton collisions at $\sqrt{s}
=$ 1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {11},
Pages = {112006},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.112006},
Abstract = {We describe a measurement of the top quark mass from events
produced in p anti-p collisions at a center-of-mass energy
of 1.96 TeV, using the Collider Detector at Fermilab. We
identify tt-bar candidates where both W bosons from the top
quarks decay into leptons (e mu, mu nu, or tau nu) from a
data sample of 360 pb-1. The top quark mass is reconstructed
in each event separately by three different methods, which
draw upon simulated distributions of the neutrino
pseudorapi+dity, tt-bar longitudinal momentum, or neutrino
azimuthal angle in order to extract probability
distributions for the top quark mass. For each method,
representative mass distributions, or templates, are
constructed from simulated samples of signal and background
events, and parametrized templates is then performed on the
data sample masses in order to derive a final top quark
mass. Combining the three template methods, taking into
account correlations in their statistical and systematic
uncertainties, results in a top quark mass measurement of
170.1 +/- 6.0 (stat.) +/- 4.1 (syst.) GeV/c2.},
Doi = {10.1103/PhysRevD.73.112006},
Key = {fds308124}
}
@article{fds307985,
Author = {Aaltonen, T and others},
Title = {Measurement of the top quark mass using the invariant mass
of lepton pairs in soft muon b-tagged events},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {5},
Pages = {051104},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.051104},
Abstract = {We present the first measurement of the mass of the top
quark in a sample of tt̅ →ℓν̅ bb̅ qq̅ events (where
ℓ=e,μ) selected by identifying jets containing a muon
candidate from the semileptonic decay of heavy-flavor
hadrons (soft muon b tagging). The pp̅ collision data used
correspond to an integrated luminosity of 2 fb-1 and
were collected by the CDF II detector at the Fermilab
Tevatron Collider. The measurement is based on a novel
technique exploiting the invariant mass of a subset of the
decay particles, specifically the lepton from the W boson of
the t→Wb decay and the muon from a semileptonic b decay.
We fit template histograms, derived from simulation of tt̅
events and a modeling of the background, to the mass
distribution observed in the data and measure a top quark
mass of 180.5 ± 12.0(stat) ±
3.6(syst) GeV/c2, consistent with the current world
average value.},
Doi = {10.1103/PhysRevD.80.051104},
Key = {fds307985}
}
@article{fds307959,
Author = {al, AVKWTAE and Collaboration, CDF},
Title = {Measurement of the top quark mass with dilepton events
selected using neuroevolution at CDF},
Journal = {Physical Review Letters},
Volume = {102},
Number = {152001},
Pages = {6},
Year = {2009},
Month = {Spring},
Key = {fds307959}
}
@article{fds308113,
Author = {Abulencia, and A, and others},
Title = {Measurement of the top quark mass with the dynamical
likelihood method using lepton plus jets events with b-tags
in $p\bar{p}$ collisions at $\sqrt{s} =$
1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.092002},
Abstract = {This report describes a measurement of the top quark mass,
M_top, with the dynamical likelihood method (DLM) using the
CDF II detector at the Fermilab Tevatron. The Tevatron
produces top/anti-top (t anti-t) pairs in p anti-p
collisions at a center-of-mass energy of 1.96 TeV. The data
sample used in this analysis was accumulated from March 2002
through August 2004, which corresponds to an integrated
luminosity of 318 pb-1. We use the tt-bar candidates in the
``epton+jets'' decay channel, requiring at least one jet
identified as a b quark by finding a displaced secondary
vertex. The DLM defines a likelihood for each event based on
the differential cross section s a function of M_top per
unit phase space volume of the final partons, multiplied by
the transfer functions from jet to parton energies. The
method takes into account all possible jet combinations in
an event, and the likelihood is multiplied event by event to
derive the top quark mass by the maximum likelihood method.
Using 63 tt-bar candidates observed in the data, with 9.2
events expected from background, we measure the top quark
mass to be 173.2+2.6_-2.4 (stat.) +/- 3.2 (syst.) GeV/c2, or
173+4.1_-4.0 GeV/c2.},
Doi = {10.1103/PhysRevD.73.092002},
Key = {fds308113}
}
@article{fds307722,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
Title = {Measurement of the top quark mass with the template method
in the [Formula: see text] channel using ATLAS
data.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {72},
Number = {6},
Pages = {2046},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2046-6},
Abstract = {The top quark mass has been measured using the template
method in the [Formula: see text] channel based on data
recorded in 2011 with the ATLAS detector at the LHC. The
data were taken at a proton-proton centre-of-mass energy of
[Formula: see text] and correspond to an integrated
luminosity of 1.04 fb<sup>-1</sup>. The analyses in the
<i>e</i>+jets and <i>μ</i>+jets decay channels yield
consistent results. The top quark mass is measured to be
<i>m</i><sub>top</sub>=174.5±0.6<sub>stat</sub>±2.3<sub>syst</sub>
GeV.},
Doi = {10.1140/epjc/s10052-012-2046-6},
Key = {fds307722}
}
@article{fds307790,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós,
G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi,
F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans,
G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
J and Colombo, T},
Title = {Measurement of the top quark pair cross section with ATLAS
in pp collisions at s=7 TeV using final states with an
electron or a muon and a hadronically decaying τ
lepton},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {717},
Number = {1-3},
Pages = {89-108},
Publisher = {Elsevier BV},
Year = {2012},
url = {http://dx.doi.org/10.1016/j.physletb.2012.09.032},
Abstract = {A measurement of the cross section of top quark pair
production in proton-proton collisions recorded with the
ATLAS detector at the Large Hadron Collider at a
centre-of-mass energy of 7 TeV is reported. The data sample
used corresponds to an integrated luminosity of 2.05 fb-1.
Events with an isolated electron or muon and a τ lepton
decaying hadronically are used. In addition, a large missing
transverse momentum and two or more energetic jets are
required. At least one of the jets must be identified as
originating from a b quark. The measured cross section,
σtt-=186±13(stat.)±20(syst.)±7(lumi.) pb, is in good
agreement with the Standard Model prediction. © 2012
CERN.},
Doi = {10.1016/j.physletb.2012.09.032},
Key = {fds307790}
}
@article{fds307551,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
S},
Title = {Measurement of the top quark pair production charge
asymmetry in proton-proton collisions at √s = 7 TeV using
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {2},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP02(2014)107},
Abstract = {This paper presents a measurement of the top quark pair
(tt̄) production charge asymmetry AC using 4.7 fb-1 of
proton-proton collisions at a centre-of-mass energy √s =
7TeV collected by the ATLAS detector at the LHC. A
tt̄-enriched sample of events with a single lepton
(electron or muon), missing transverse momentum and at least
four high transverse momentum jets, of which at least one is
tagged as coming from a b-quark, is selected. A likelihood
fit is used to reconstruct the tt̄ event kinematics. A
Bayesian unfolding procedure is employed to estimate AC at
the parton-level. The measured value of the tt̄ production
charge asymmetry is AC = 0.006 ± 0.010, where the
uncertainty includes both the statistical and the systematic
components. Differential AC measurements as a function of
the invariant mass, the rapidity and the transverse momentum
of the tt̄- system are also presented. In addition, AC is
measured for a subset of events with large tt̄ velocity,
where physics beyond the Standard Model could contribute.
All measurements are consistent with the Standard Model
predictions.},
Doi = {10.1007/JHEP02(2014)107},
Key = {fds307551}
}
@article{fds307749,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the top quark pair production cross section
in pp collisions at √s=7TeV in dilepton final states with
ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {707},
Number = {5},
Pages = {459-477},
Publisher = {Elsevier BV},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2011.12.055},
Abstract = {A measurement of the production cross section of top quark
pairs (tt̄) in proton-proton collisions at a center-of-mass
energy of 7 TeV recorded with the ATLAS detector at the
Large Hadron Collider is reported. Candidate events are
selected in the dilepton topology with large missing
transverse energy and at least two jets. Using a data sample
corresponding to an integrated luminosity of 35pb-1, a tt̄
production cross section σtt̄=177±20(stat.)±14(syst.)±7(lum.)pb
is measured for an assumed top quark mass of mt=172.5GeV. A
second measurement requiring at least one jet identified as
coming from a b quark yields a comparable result,
demonstrating that the dilepton final states are consistent
with being accompanied by b-quark jets. These measurements
are in good agreement with Standard Model predictions. ©
2011 CERN.},
Doi = {10.1016/j.physletb.2011.12.055},
Key = {fds307749}
}
@article{fds308215,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Signore, KD and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Loreto, GD and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Geld, TL and II, RJG and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Gobbi, B and Gómez, B and Gómez, G and Goncharov, PI and Solís, JLG and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Grannis, PD and Green, DR and Greenlee, H and Grinstein, S and Grudberg, P and Grünendahl, S and Guglielmo, G and Guida, JA and Guida, JM and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hedin, D and Heinson, AP and Heintz, U and Hernández-Monloya, R and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hsieh, F and Hu, T and Ito, AS and Jaques,
J and Jerger, SA and Jesik, R and Joffe-Minor, T and Johns, K and Johnson,
M and Jonckheere, A and Jones, M and Jöstlein, H and Jun, SY and Jung, CK and Kahn, S and Kalbfleisch, G and Karmanov, D and Karmgard, D and Kehoe, R and Kelly, ML and Kim, SK and Klima, B and Klopfenstein, C and Ko, W and Kohli,
JM and Koltick, D and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kuleshov, S and Kulik, Y and Kunori, S and Landry,
F and Landsberg, G and Lauer, B and Leflat, A and Li, J and Li, QZ and Lima,
JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lobkowicz, F and Loken, SC and Lucotte, A and Lueking, L and Lyon, AL and Maciel, AKA and Madaras, RJ and Madden, R and Magaña-Mendoza, L and Manankov, V and Mani, S and Mao, HS and Markeloff, R and Marshall, T and Martin, MI and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald, J and McKibben, T and McKinley, J and McMahon, T and Melanson,
HL and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mincer,
A and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Mooney, P and Moromisato, J and Mostafa, M and Motta, HD and Murphy, C and Nang, F and Narain, M and Narasimham, VS and Narayanan, A and Neal, HA and Negret, JP and Nemethy, P and Norman, D and Oesch, L and Oguri, V and Oliveira, E and Oltman, E and Oshima, N and Owen, D and Padley, P and Para,
A and Park, YM and Partridge, R and Parua, N and Paterno, M and Pawlik, B and Perkins, J and Peters, M and Piegaia, R and Piekarz, H and Pischalnikov,
Y and Pope, BG and Prosper, HB and Protopopescu, S and Qian, J and Quintas,
PZ and Raja, R and Rajagopalan, S and Ramirez, O and Reucroft, S and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Sánchez-Hernández, A and Santoro, A and Sawyer,
L and Schamberger, RD and Schellman, H and Sculli, J and Shabalina, E and Shaffer, C and Shankar, HC and Shivpuri, RK and Shpakov, D and Shupe, M and Singh, H and Singh, JB and Sirotenko, V and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sosebee, M and Sotnikova, N and Souza, M and Steinbrück, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink,
M and Sznajder, A and Tamburello, P and Tarazi, J and Tartaglia, M and Thomas, TLT and Thompson, J and Trippe, TG and Tuts, PM and Vaniev, V and Varelas, N and Varnes, EW and Vititoe, D and Volkov, AA and Vorobiev,
AP and Wahl, HD and Wang, G and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Wightman, JA and Willis, S and Wimpenny, SJ and Wirjawan, JVD and Womersley, J and Won, E and Wood, DR and Wu, Z and Yamada, R and Yamin, P and Yasuda, T and Yepes, P and Yip, K and Yoshikawa, C and Youssef, S and Yu, J and Yu, Y and Zhang, B and Zhou, Y and Zhou, Z and Zhu, ZH and Zielinski, M and Zieminska, D and Zieminski, A and Zverev, EG and Zylberstejn, A},
Title = {Measurement of the top quark pair production cross section
in pp̄ collisions using multijet final states},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {1},
Pages = {1-26},
Year = {1999},
url = {http://dx.doi.org/10.1103/PhysRevD.60.012001},
Abstract = {We have studied tt̄ production using multijet final states
in pp̄ collisions at a center-of-mass energy of 1.8 TeV,
with an integrated luminosity of 110.3 pb-1. Each of the top
quarks with these final states decays exclusively to a
bottom quark and a W boson, with the W bosons decaying into
quark-antiquark pairs. The analysis has been optimized using
neural networks to achieve the smallest expected fractional
uncertainty on the tt̄ production cross section, and yields
a cross section of 7.1±2.8 (stat)±1.5 (syst) pb, assuming
a top quark mass of 172.1 GeV/c2. Combining this result with
previous DØ measurements, where one or both of the W bosons
decay leptonically, gives a tt̄ production cross section of
5.9±1.2 (stat)±1.1 (syst) pb. ©1999 The American Physical
Society.},
Doi = {10.1103/PhysRevD.60.012001},
Key = {fds308215}
}
@booklet{Abachi97b,
Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cumings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard, J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G},
Title = {Measurement of the top quark pair production cross section
in p¯p collisions},
Journal = {Physical Review Letters},
Volume = {79},
Number = {7},
Pages = {1203-1208},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.1203},
Abstract = {We present a measurement of the t¯t production cross
section in p¯p collisions at √s=1.8TeV by the D0
experiment at the Fermilab Tevatron. The measurement is
based on data from an integrated luminosity of approximately
125pb−1 accumulated during the 1992–1996 collider run.
We observe 39 t¯t candidate events in the dilepton and
lepton+jets decay channels with an expected background of
13.7 ± 2.2 events. For a top quark mass of 173.3 GeV/c2, we
measure the t¯t production cross section to be 5.5 ± 1.8
pb. © 1997 The American Physical Society.},
Doi = {10.1103/PhysRevLett.79.1203},
Key = {Abachi97b}
}
@article{fds308223,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del-Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Measurement of the top quark pair production cross section
in the all-jets decay channel},
Journal = {Physical Review Letters},
Volume = {83},
Number = {10},
Pages = {1908-1913},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.83.1908},
Abstract = {We present a measurement of t¯t production in p¯p
collisions at √s = 1.8TeV from 110pb-1 of data collected
in the all-jets decay channel with the D0 detector at
Fermilab. A neural network analysis yields a cross section
of 7.1 ± 2.8(stat) ± 1.5(syst)pb at a top quark mass (mt)
of 172.1GeV/c2. Using previous D0 measurements from dilepton
and single lepton channels, the combined D0 result for the
t¯t production cross section is 5.9 ± 1.2(stat) ±
1.1(syst)pb for mt = 172.1GeV/c2. © 1999 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.83.1908},
Key = {fds308223}
}
@article{fds307766,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma,
Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou,
H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri,
AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa,
HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
N and Benhammou, Y and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse,
M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Measurement of the top quark pair production cross-section
with ATLAS in the single lepton channel},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {711},
Number = {3-4},
Pages = {244-263},
Publisher = {Elsevier BV},
Year = {2012},
url = {http://dx.doi.org/10.1016/j.physletb.2012.03.083},
Abstract = {A measurement of the production cross-section for top quark
pairs (tt-) in pp collisions at s=7TeV is presented using
data recorded with the ATLAS detector at the Large Hadron
Collider. Events are selected in the single lepton topology
by requiring an electron or muon, large missing transverse
momentum and at least three jets. With a data sample of 35
pb -1, two different multivariate methods, one of which uses
b-quark jet identification while the other does not, use
kinematic variables to obtain cross-section measurements of
σtt-=187±11(stat.)-17+18(syst.)±6(lumi.)pb and
σtt-=173±17(stat.)-16+18(syst.)±6(lumi.)pb respectively.
The two measurements are in agreement with each other and
with QCD calculations. The first measurement has a better a
priori sensitivity and constitutes the main result of this
Letter. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.03.083},
Key = {fds307766}
}
@article{fds308058,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the top-quark mass in all-hadronic decays in
p anti-p collisions at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {14},
Pages = {142001},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.142001},
Abstract = {We present a measurement of the top-quark mass Mtop in the
all-hadronic decay channel t[overline t]-->W+bW-[overline
b]-->q1[overline q]2bq3[overline q]4[overline b]. The
analysis is performed using 310 pb-1 of sqrt(s)=1.96 TeV
p[overline p] collisions collected with the CDF II detector
using a multijet trigger. The mass measurement is based on
an event-by-event likelihood which depends on both the
sample purity and the value of the top-quark mass, using 90
possible jet-to-parton assignments in the six-jet final
state. The joint likelihood of 290 selected events yields a
value of Mtop=177.1$\pm$4.9(stat)$\pm$4.7(syst)
GeV/c2.},
Doi = {10.1103/physrevlett.98.142001},
Key = {fds308058}
}
@article{fds310349,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of the top-quark mass in the all-hadronic
channel using the full CDF data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.90.091101},
Abstract = {The top-quark mass Mtop is measured using top
quark-antiquark pairs produced in proton-antiproton
collisions at a center-of-mass energy of 1.96 TeV and that
decay into a fully hadronic final state. The full data set
collected with the CDF II detector at the Fermilab Tevatron
Collider, corresponding to an integrated luminosity of
9.3fb-1, is used. Events are selected that have six to eight
jets, at least one of which is identified as having
originated from a b quark. In addition, a multivariate
algorithm, containing multiple kinematic variables as
inputs, is used to discriminate signal events from
background events due to QCD multijet production. Templates
for the reconstructed top-quark mass are combined in a
likelihood fit to measure Mtop with a simultaneous
calibration of the jet energy scale. A value of
Mtop=175.07±1.19(stat)-1.58+1.55(syst)GeV/c2 is obtained
for the top-quark mass.},
Doi = {10.1103/PhysRevD.90.091101},
Key = {fds310349}
}
@article{fds310323,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin,
V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Measurement of the top-quark mass in the fully hadronic
decay channel from ATLAS data at [Formula: see
text].},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {4},
Pages = {158},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3373-1},
Abstract = {The mass of the top quark is measured in a data set
corresponding to 4.6 [Formula: see text] of proton-proton
collisions with centre-of-mass energy [Formula: see
text] TeV collected by the ATLAS detector at the LHC.
Events consistent with hadronic decays of top-antitop quark
pairs with at least six jets in the final state are
selected. The substantial background from multijet
production is modelled with data-driven methods that utilise
the number of identified [Formula: see text]-quark jets and
the transverse momentum of the sixth leading jet, which have
minimal correlation. The top-quark mass is obtained from
template fits to the ratio of three-jet to dijet mass. The
three-jet mass is calculated from the three jets produced in
a top-quark decay. Using these three jets the dijet mass is
obtained from the two jets produced in the [Formula: see
text] boson decay. The top-quark mass obtained from this fit
is thus less sensitive to the uncertainty in the energy
measurement of the jets. A binned likelihood fit yields a
top-quark mass of [Formula: see text].},
Doi = {10.1140/epjc/s10052-015-3373-1},
Key = {fds310323}
}
@article{fds307870,
Author = {Aaltonen, TEA},
Title = {Measurement of the top-quark mass in the lepton+jets channel
using a matrix element technique with the {CDF II}
detector},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {7},
Pages = {071105},
Publisher = {American Physical Society},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.84.071105},
Abstract = {A measurement of the top-quark mass is presented using
Tevatron data from proton-antiproton collisions at
center-of-mass energy √s=1.96TeV collected with the CDF II
detector. Events are selected from a sample of candidates
for production of tt̄ pairs that decay into the lepton+jets
channel. The top-quark mass is measured with an unbinned
maximum likelihood method where the event probability
density functions are calculated using signal and background
matrix elements, as well as a set of parametrized
jet-to-parton transfer functions. The likelihood function is
maximized with respect to the top-quark mass, the signal
fraction in the sample, and a correction to the jet energy
scale (JES) calibration of the calorimeter jets. The
simultaneous measurement of the JES correction (ΔJES)
amounts to an additional in situ jet energy calibration
based on the known mass of the hadronically decaying W
boson. Using the data sample of 578 lepton+jets candidate
events, corresponding to 3.2fb-1 of integrated luminosity,
the top-quark mass is measured to be mt=172.4±1.4(stat+ΔJES)±1.
3(syst)GeV/c2. © 2011 American Physical
Society.},
Doi = {10.1103/PhysRevD.84.071105},
Key = {fds307870}
}
@article{fds310270,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of the top-quark mass in the tt¯ dilepton
channel using the full CDF Run II data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.92.032003},
Abstract = {We present a measurement of the top-quark mass in events
containing two leptons (electrons or muons) with a large
transverse momentum, two or more energetic jets, and a
transverse-momentum imbalance. We use the full
proton-antiproton collision data set collected by the CDF
experiment during the Fermilab Tevatron Run II at
center-of-mass energy s=1.96 TeV, corresponding to an
integrated luminosity of 9.1 fb-1. A special observable is
exploited for an optimal reduction of the dominant
systematic uncertainty, associated with the knowledge of the
absolute energy of the hadronic jets. The distribution of
this observable in the selected events is compared to
simulated distributions of tt¯ dilepton signal and
background. We measure a value for the top-quark mass of
171.5±1.9 (stat)±2.5 (syst) GeV/c2.},
Doi = {10.1103/PhysRevD.92.032003},
Key = {fds310270}
}
@article{fds356565,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Akesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Bella,
LA and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Measurement of the top-quark mass in tt¯ + 1-jet events
collected with the ATLAS detector in pp collisions at √s =
8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {11},
Year = {2019},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2019)150},
Abstract = {A determination of the top-quark mass is presented using
20.2 fb−1 of 8 TeV proton-proton collision data produced
by the Large Hadron Collider and collected by the ATLAS
experiment. The normalised differential cross section of
top-quark pair production in association with an energetic
jet is measured in the lepton+jets final state and unfolded
to parton and particle levels. The unfolded distribution at
parton level can be described using next-to-leading-order
QCD predictions in terms of either the top-quark pole mass
or the running mass as defined in the (modified) minimal
subtraction scheme. A comparison between the experimental
distribution and the theoretical prediction allows the
top-quark mass to be extracted in the two schemes. The value
obtained for the pole-mass scheme is: mtpole=171.1±0.4(stat)±0.9(syst)−0.3+0.7(theo)GeV
The extracted value in the running-mass scheme is:
mt(mt)=162.9±0.5(stat)±1.0(syst)−1.2+2.1(theo)GeV. The
results for the top-quark mass using the two schemes are
consistent, when translated from one scheme to the other.
[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP11(2019)150},
Key = {fds356565}
}
@article{fds308063,
Author = {Aaltonen, and T, and others},
Title = {Measurement of the top-quark mass using missing $E_T$ + jets
events with secondary vertex $b-$tagging at CDF
II},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {11},
Pages = {111103},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.111103},
Abstract = {We present a measurement of the top-quark mass in p[overline
p] collisions at sqrt(s)=1.96 TeV which uses events with an
inclusive signature of missing transverse energy and jets.
The event selection is sensitive to t[overline
t]-->W+bW-[overline b]-->lnubqq[prime][overline b]
independent of the lepton flavor and results in a large
acceptance for W-->taunu decays. All-hadronic t[overline t]
decays and events with identified electrons or muons are
vetoed to provide a statistically independent sample with
respect to all previous measurements. The top-quark mass is
inferred from the distribution of the scalar sum of all jet
transverse energies and the missing transverse energy. Using
311 pb-1 of integrated luminosity recorded by the Collider
Detector at Fermilab, we measure a top-quark mass
mt=172.3-9.6+10.8(stat)$\pm$10.8(syst) GeV/c2. While the
uncertainty on mt is larger than that of other measurements,
the result is statistically uncorrelated with those of other
methods and thus can help to reduce the overall mt
uncertainty when combined with other existing
measurements.},
Doi = {10.1103/PhysRevD.75.111103},
Key = {fds308063}
}
@article{fds307954,
Author = {Aaltonen, T and others},
Title = {Measurement of the Top-Quark Mass with Dilepton Events
Selected Using Neuroevolution at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {15},
Pages = {152001},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.152001},
Abstract = {We present an analysis of the mass of the X(3872)
reconstructed via its decay to J/ψπ+π- using
2.4 fb-1 of integrated luminosity from pp̅ collisions
at sqrt[s]=1.96 TeV, collected with the CDF II detector
at the Fermilab Tevatron. The possible existence of two
nearby mass states is investigated. Within the limits of our
experimental resolution the data are consistent with a
single state, and having no evidence for two states we set
upper limits on the mass difference between two hypothetical
states for different assumed ratios of contributions to the
observed peak. For equal contributions, the 95% confidence
level upper limit on the mass difference is 3.6 MeV/c2.
Under the single-state model the X(3872) mass is measured to
be 3871.61$\pm$0.16(stat)$\pm$0.19(syst) MeV/c2, which
is the most precise determination to date.},
Doi = {10.1103/physrevlett.102.152001},
Key = {fds307954}
}
@article{fds307563,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Measurement of the top-quark pair-production cross section
in events with two leptons and bottom-quark jets using the
full CDF data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.88.091103},
Abstract = {We present a measurement of the top-quark pair production
cross section in proton-antiproton collisions at √s=1.96
TeV. The data were collected at the Fermilab Tevatron by the
CDF II detector and correspond to an integrated luminosity
of 8.8 fb-1, representing the complete CDF Run II data set.
We select events consistent with the production of top-quark
pairs by requiring the presence of two reconstructed
leptons, an imbalance in the total event transverse
momentum, and jets. At least one jet is required to be
identified as consistent with the fragmentation of a bottom
quark using a secondary-vertex-finding algorithm. The 246
candidate events are estimated to have a signal purity of
91%. We measure a cross section of σ tt̄=7.09±0.84 pb,
assuming a top-quark mass of 172.5 GeV/c2. The results are
consistent with the standard model as predicted by
next-to-leading-order calculations. Published by the
American Physical Society.},
Doi = {10.1103/PhysRevD.88.091103},
Key = {fds307563}
}
@article{fds371119,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Measurement of the total cross section and ρ -parameter
from elastic scattering in pp collisions at √s=13 TeV with
the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11436-8},
Abstract = {In a special run of the LHC with β⋆= 2.5 km,
proton–proton elastic-scattering events were recorded at
s=13 TeV with an integrated luminosity of 340μb-1 using the
ALFA subdetector of ATLAS in 2016. The elastic cross section
was measured differentially in the Mandelstam t variable in
the range from - t= 2.5 · 10 - 4 GeV 2 to - t= 0.46 GeV 2
using 6.9 million elastic-scattering candidates. This paper
presents measurements of the total cross section σtot ,
parameters of the nuclear slope, and the ρ -parameter
defined as the ratio of the real part to the imaginary part
of the elastic-scattering amplitude in the limit t→ 0 .
These parameters are determined from a fit to the
differential elastic cross section using the optical theorem
and different parameterizations of the t-dependence. The
results for σtot and ρ are σtot(pp→X)=104.7±1.1mb,ρ=0.098±0.011.
The uncertainty in σtot is dominated by the luminosity
measurement, and in ρ by imperfect knowledge of the
detector alignment and by modelling of the nuclear
amplitude.},
Doi = {10.1140/epjc/s10052-023-11436-8},
Key = {fds371119}
}
@article{fds313586,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurement of the total cross section from elastic
scattering in pp collisions at √s=7 TeV with the ATLAS
detector},
Journal = {Nuclear Physics B},
Volume = {889},
Pages = {486-548},
Publisher = {Elsevier BV},
Year = {2014},
Month = {December},
ISSN = {0550-3213},
url = {http://dx.doi.org/10.1016/j.nuclphysb.2014.10.019},
Abstract = {A measurement of the total pp cross section at the LHC at
s=7 TeV is presented. In a special run with high-β⋆ beam
optics, an integrated luminosity of 80 μb−1 was
accumulated in order to measure the differential elastic
cross section as a function of the Mandelstam momentum
transfer variable t. The measurement is performed with the
ALFA sub-detector of ATLAS. Using a fit to the differential
elastic cross section in the |t| range from 0.01 GeV2 to 0.1
GeV2 to extrapolate to |t|→0, the total cross section,
σtot(pp→X), is measured via the optical theorem to be:
σtot(pp→X)=95.35±0.38(stat.)±1.25(exp.)±0.37(extr.)mb,
where the first error is statistical, the second accounts
for all experimental systematic uncertainties and the last
is related to uncertainties in the extrapolation to |t|→0.
In addition, the slope of the elastic cross section at small
|t| is determined to be B=19.73±0.14(stat.)±0.26(syst.)
GeV−2.},
Doi = {10.1016/j.nuclphysb.2014.10.019},
Key = {fds313586}
}
@article{fds321082,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the total cross section from elastic
scattering in pp collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {761},
Pages = {158-178},
Publisher = {Elsevier BV},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.020},
Abstract = {A measurement of the total pp cross section at the LHC at
s=8 TeV is presented. An integrated luminosity of 500
μb−1 was accumulated in a special run with high-β⋆
beam optics to measure the differential elastic cross
section as a function of the Mandelstam momentum transfer
variable t. The measurement is performed with the ALFA
sub-detector of ATLAS. Using a fit to the differential
elastic cross section in the −t range from 0.014 GeV2 to
0.1 GeV2 to extrapolate t→0, the total cross section,
σtot(pp→X), is measured via the optical theorem to be
σtot(pp→X)=96.07±0.18(stat.)±0.85(exp.)±0.31(extr.)mb,
where the first error is statistical, the second accounts
for all experimental systematic uncertainties and the last
is related to uncertainties in the extrapolation t→0. In
addition, the slope of the exponential function describing
the elastic cross section at small t is determined to be
B=19.74±0.05(stat.)±0.23(syst.)GeV−2.},
Doi = {10.1016/j.physletb.2016.08.020},
Key = {fds321082}
}
@article{fds316853,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Measurement of the transverse momentum and [Formula: see
text] distributions of Drell-Yan lepton pairs in
proton-proton collisions at [Formula: see text] TeV with
the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {291},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4070-4},
Abstract = {Distributions of transverse momentum [Formula: see text] and
the related angular variable [Formula: see text] of
DrellΓÇôYan lepton pairs are measured in
20.3 fb[Formula: see text] of proton–proton
collisions at [Formula: see text] TeV with the ATLAS
detector at the LHC. Measurements in electron-pair and
muon-pair final states are corrected for detector effects
and combined. Compared to previous measurements in
protonΓÇôproton collisions at [Formula: see
text] TeV, these new measurements benefit from a larger
data sample and improved control of systematic
uncertainties. Measurements are performed in bins of
lepton-pair mass above, around and below the <i>Z</i>-boson
mass peak. The data are compared to predictions from
perturbative and resummed QCD calculations. For values of
[Formula: see text] the predictions from the Monte Carlo
generator ResBos are generally consistent with the data
within the theoretical uncertainties. However, at larger
values of [Formula: see text] this is not the case. Monte
Carlo generators based on the parton-shower approach are
unable to describe the data over the full range of [Formula:
see text] while the fixed-order prediction of Dynnlo falls
below the data at high values of [Formula: see text]. ResBos
and the parton-shower Monte Carlo generators provide a much
better description of the evolution of the [Formula: see
text] and [Formula: see text] distributions as a function of
lepton-pair mass and rapidity than the basic shape of the
data.},
Doi = {10.1140/epjc/s10052-016-4070-4},
Key = {fds316853}
}
@article{fds351090,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler,
A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso,
S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Araque, JP and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Measurement of the transverse momentum distribution of
Drell–Yan lepton pairs in proton–proton collisions at
√s=13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {7},
Year = {2020},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8001-z},
Abstract = {This paper describes precision measurements of the
transverse momentum pTℓℓ (ℓ= e, μ) and of the angular
variable ϕη∗ distributions of Drell–Yan lepton pairs
in a mass range of 66–116 GeV. The analysis uses data
from 36.1 fb- 1 of proton–proton collisions at a
centre-of-mass energy of s=13TeV collected by the ATLAS
experiment at the LHC in 2015 and 2016. Measurements in
electron-pair and muon-pair final states are performed in
the same fiducial volumes, corrected for detector effects,
and combined. Compared to previous measurements in
proton–proton collisions at s=7 and 8TeV, these new
measurements probe perturbative QCD at a higher
centre-of-mass energy with a different composition of
initial states. They reach a precision of 0.2% for the
normalized spectra at low values of pTℓℓ. The data are
compared with different QCD predictions, where it is found
that predictions based on resummation approaches can
describe the full spectrum within uncertainties.},
Doi = {10.1140/epjc/s10052-020-8001-z},
Key = {fds351090}
}
@article{fds307758,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the transverse momentum distribution of W
bosons in pp collisions at √s=7TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012005},
Abstract = {This paper describes a measurement of the W boson transverse
momentum distribution using ATLAS pp collision data from the
2010 run of the LHC at √s=7TeV, corresponding to an
integrated luminosity of about 31pb -1. Events form both
W→eν and W→μν are used, and the transverse momentum
of the W candidates is measured through the energy
deposition in the calorimeter from the recoil of the W. The
resulting distributions are unfolded to obtain the
normalized differential cross sections as a function of the
W boson transverse momentum. We present results for
pTW<300GeV in the electron and muon channels as well as for
their combination, and compare the combined results to the
predictions of perturbative QCD and a selection of event
generators. © 2012 CERN.},
Doi = {10.1103/PhysRevD.85.012005},
Key = {fds307758}
}
@article{fds307861,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Measurement of the transverse momentum distribution of
Z/γ* bosons in proton-proton collisions at s=7
TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {705},
Number = {5},
Pages = {415-434},
Publisher = {Elsevier BV},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2011.10.018},
Abstract = {A measurement of the Z/γ* transverse momentum (pTZ)
distribution in proton-proton collisions at s=7 TeV is
presented using Z/γ*→e+e- and Z/γ*→μ+μ- decays
collected with the ATLAS detector in data sets with
integrated luminosities of 35 pb-1 and 40 pb-1,
respectively. The normalized differential cross sections are
measured separately for electron and muon decay channels as
well as for their combination up to pTZ of 350 GeV for
invariant dilepton masses 66 GeV<mℓℓ<116 GeV. The
measurement is compared to predictions of perturbative QCD
and various event generators. The prediction of resummed QCD
combined with fixed order perturbative QCD is found to be in
good agreement with the data. © 2011 CERN.},
Doi = {10.1016/j.physletb.2011.10.018},
Key = {fds307861}
}
@article{fds310304,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurement of the transverse polarization of Λ and Λ ¯
hyperons produced in proton-proton collisions at √s = 7
TeV using the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.91.032004},
Abstract = {The transverse polarization of Λ and Λ¯ hyperons produced
in proton-proton collisions at a center-of-mass energy of 7
TeV is measured. The analysis uses 760 μb-1 of minimum bias
data collected by the ATLAS detector at the LHC in the year
2010. The measured transverse polarization averaged over
Feynman xF from 5×10-5 to 0.01 and transverse momentum pT
from 0.8 to 15 GeV is -0.010±0.005(stat)±0.004(syst) for
Λ and 0.002±0.006(stat)±0.004(syst) for Λ¯. It is also
measured as a function of xF and pT, but no significant
dependence on these variables is observed. Prior to this
measurement, the polarization was measured at fixed-target
experiments with center-of-mass energies up to about 40 GeV.
The ATLAS results are compatible with the extrapolation of a
fit from previous measurements to the xF range covered by
this measurement.},
Doi = {10.1103/PhysRevD.91.032004},
Key = {fds310304}
}
@article{fds375335,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Aktas, S and Al Khoury and K and Alberghi,
GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Alegria, ZL and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Measurement of the tt¯ cross section and its ratio to the Z
production cross section using pp collisions at s=13.6 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {848},
Pages = {138376-138376},
Publisher = {Elsevier BV},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138376},
Abstract = {The inclusive top-quark-pair production cross section σtt¯
and its ratio to the Z-boson production cross section have
been measured in proton–proton collisions at s=13.6 TeV,
using 29 fb−1 of data collected in 2022 with the ATLAS
experiment at the Large Hadron Collider. Using events with
an opposite-charge electron-muon pair and b-tagged jets, and
assuming Standard Model decays, the top-quark-pair
production cross section is measured to be
σtt¯=850±3(stat.)±18(syst.)±20(lumi.) pb. The ratio of
the tt¯ and the Z-boson production cross sections is also
measured, where the Z-boson contribution is determined for
inclusive e+e− and μ+μ− events in a fiducial phase
space. The relative uncertainty on the ratio is reduced
compared to the tt¯ cross section, thanks to the
cancellation of several systematic uncertainties. The result
for the ratio, Rtt¯/Z=1.145±0.003(stat.)±0.021(syst.)±0.002(lumi.)
is consistent with the Standard Model prediction using the
PDF4LHC21 PDF set.},
Doi = {10.1016/j.physletb.2023.138376},
Key = {fds375335}
}
@article{fds350336,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Araque, JP and Ferraz, VA and Pereira,
RA},
Title = {Measurement of the tt¯ production cross-section and lepton
differential distributions in eμ dilepton events from pp
collisions at √s=13TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {6},
Year = {2020},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-7907-9},
Abstract = {The inclusive top quark pair (tt¯) production cross-section
σtt¯ has been measured in proton–proton collisions at
s=13TeV, using 36.1 fb- 1 of data collected in 2015–2016
by the ATLAS experiment at the LHC. Using events with an
opposite-charge eμ pair and b-tagged jets, the
cross-section is measured to be: σtt¯=826.4±3.6(stat)±11.5(syst)±15.7(lumi)±1.9(beam)pb,where
the uncertainties reflect the limited size of the data
sample, experimental and theoretical systematic effects, the
integrated luminosity, and the LHC beam energy, giving a
total uncertainty of 2.4%. The result is consistent with
theoretical QCD calculations at next-to-next-to-leading
order. It is used to determine the top quark pole mass via
the dependence of the predicted cross-section on mtpole,
giving mtpole=173.1-2.1+2.0GeV. It is also combined with
measurements at s=7TeV and s=8TeV to derive ratios and
double ratios of tt¯ and Z cross-sections at different
energies. The same event sample is used to measure absolute
and normalised differential cross-sections as functions of
single-lepton and dilepton kinematic variables, and the
results are compared with predictions from various Monte
Carlo event generators.},
Doi = {10.1140/epjc/s10052-020-7907-9},
Key = {fds350336}
}
@article{fds310328,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the tt¯ production cross-section as a
function of jet multiplicity and jet transverse momentum in
7 TeV proton-proton collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {1},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2015)020},
Abstract = {Abstract: The tt¯$$ t\overline{t} $$ production
cross-section dependence on jet multiplicity and jet
transverse momentum is reported for proton-proton collisions
at a centre-of-mass energy of 7 TeV in the single-lepton
channel. The data were collected with the ATLAS detector at
the CERN Large Hadron Collider and comprise the full 2011
data sample corresponding to an integrated luminosity of 4.6
fb−1. Differential cross-sections are presented as a
function of the jet multiplicity for up to eight jets using
jet transverse momentum thresholds of 25, 40, 60, and 80
GeV, and as a function of jet transverse momentum up to the
fifth jet. The results are shown after background
subtraction and corrections for all known detector effects,
within a kinematic range closely matched to the experimental
acceptance. Several QCD-based Monte Carlo models are
compared with the results. Sensitivity to the parton shower
modelling is found at the higher jet multiplicities, at high
transverse momentum of the leading jet and in the transverse
momentum spectrum of the fifth leading jet. The
MC@NLO+HERWIG MC is found to predict too few events at
higher jet multiplicities.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP01(2015)020},
Key = {fds310328}
}
@article{fds352890,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Measurement of the tt¯ production cross-section in the
lepton+jets channel at s=13 TeV with the ATLAS
experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {810},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2020.135797},
Abstract = {The top anti-top quark production cross-section is measured
in the lepton+jets channel using proton–proton collision
data at a centre-of-mass energy of s=13 TeV collected with
the ATLAS detector at the LHC. The dataset corresponds to an
integrated luminosity of 139 fb−1. Events with exactly one
charged lepton and four or more jets in the final state,
with at least one jet containing b-hadrons, are used to
determine the tt¯ production cross-section through a
profile-likelihood fit. The inclusive cross-section is
measured to be σinc=830±0.4(stat.)±36(syst.)±14(lumi.)pb
with a relative uncertainty of 4.6%. The result is
consistent with theoretical calculations at
next-to-next-to-leading order in perturbative QCD. The
fiducial tt¯ cross-section within the experimental
acceptance is also measured.},
Doi = {10.1016/j.physletb.2020.135797},
Key = {fds352890}
}
@article{fds321132,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of the tt¯ production cross-section using eμ
events with b-tagged jets in pp collisions at √s=13TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {761},
Pages = {136-157},
Publisher = {Elsevier BV},
Year = {2016},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.019},
Abstract = {This paper describes a measurement of the inclusive top
quark pair production cross-section (σtt¯) with a data
sample of 3.2fb−1 of proton–proton collisions at a
centre-of-mass energy of s=13TeV, collected in 2015 by the
ATLAS detector at the LHC. This measurement uses events with
an opposite-charge electron–muon pair in the final state.
Jets containing b-quarks are tagged using an algorithm based
on track impact parameters and reconstructed secondary
vertices. The numbers of events with exactly one and exactly
two b-tagged jets are counted and used to determine
simultaneously σtt¯ and the efficiency to reconstruct and
b-tag a jet from a top quark decay, thereby minimising the
associated systematic uncertainties. The cross-section is
measured to be: σtt¯=818±8(stat)±27(syst)±19(lumi)±12(beam)
pb, where the four uncertainties arise from data statistics,
experimental and theoretical systematic effects, the
integrated luminosity and the LHC beam energy, giving a
total relative uncertainty of 4.4%. The result is consistent
with theoretical QCD calculations at next-to-next-to-leading
order. A fiducial measurement corresponding to the
experimental acceptance of the leptons is also
presented.},
Doi = {10.1016/j.physletb.2016.08.019},
Key = {fds321132}
}
@article{fds356726,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurement of the tt¯ γ production cross section in
proton-proton collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {11},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2017)086},
Abstract = {The cross section of a top-quark pair produced in
association with a photon is measured in proton-proton
collisions at a centre-of-mass energy of s=8 TeV with 20.2
fb−1 of data collected by the ATLAS detector at the Large
Hadron Collider in 2012. The measurement is performed by
selecting events that contain a photon with transverse
momentum pT > 15 GeV, an isolated lepton with large
transverse momentum, large missing transverse momentum, and
at least four jets, where at least one is identified as
originating from a b-quark. The production cross section is
measured in a fiducial region close to the selection
requirements. It is found to be 139 ± 7 (stat.) ± 17
(syst.) fb, in good agreement with the theoretical
prediction at next-to-leading order of 151 ± 24 fb. In
addition, differential cross sections in the fiducial region
are measured as a function of the transverse momentum and
pseudorapidity of the photon.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP11(2017)086},
Key = {fds356726}
}
@article{fds356608,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA},
Title = {Measurement of the tt¯Z and tt¯W cross sections in
proton-proton collisions at s=13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {99},
Number = {7},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.99.072009},
Abstract = {A measurement of the associated production of a top-quark
pair (tt) with a vector boson (W, Z) in proton-proton
collisions at a center-of-mass energy of 13 TeV is
presented, using 36.1 fb-1 of integrated luminosity
collected by the ATLAS detector at the Large Hadron
Collider. Events are selected in channels with two same- or
opposite-sign leptons (electrons or muons), three leptons or
four leptons, and each channel is further divided into
multiple regions to maximize the sensitivity of the
measurement. The ttZ and ttW production cross sections are
simultaneously measured using a combined fit to all regions.
The best-fit values of the production cross sections are
σttZ=0.95±0.08stat±0.10syst pb and σttW=0.87±0.13stat±0.14syst
pb in agreement with the Standard Model predictions. The
measurement of the ttZ cross section is used to set
constraints on effective field theory operators which modify
the ttZ vertex.},
Doi = {10.1103/PhysRevD.99.072009},
Key = {fds356608}
}
@article{fds313578,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canelli, F and Canepa, A and Casarsa, M and Carlsmith, D and Carosi,
R and Carron, S and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Cruz, A and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Demers,
S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and Dituro, P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Donini, J and D'Onofrio, M and Dorigo, T and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Field, RD and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii,
Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grosso-Pilcher, C and Grundler, U and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, and Marginean, R and Marino, C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic,
N and Miles, J and Miller, L and Miller, R and Miller, JS and Mills, C and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi,
N and Mohr, B and Moore, R and Morello, M and Fernandez, PAM and Muelmenstaedt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Nelson, T and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Ohsugi,
T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Osterberg,
K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou,
V and Paramonov, AA and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rahaman, MA and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray, H and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo,
T and Rolli, S and Roser, R and Rossin, R and Rott, C and Russ, J and Rusu, V and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis,
RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sill, A and Sinervo, P and Sisakyan, A and Sjolin, J and Skiba, A and Slaughter, AJ and Sliwa,
K},
Title = {Measurement of the tt̄ production cross section in pp̄
collisions at s=1.96 TeV using lepton plus jets events with
semileptonic B decays to muons},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {72},
Number = {3},
Pages = {1-20},
Publisher = {American Physical Society (APS)},
Year = {2005},
ISSN = {1550-7998},
url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000231564900007&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
Abstract = {We present a measurement of the tt̄ production cross
section using 194 pb-1 of CDF II data using events with a
high transverse momentum electron or muon, three or more
jets, and missing transverse energy. The measurement assumes
100% t→Wb branching fraction. Events consistent with tt̄
decay are found by identifying jets containing heavy-flavor
semileptonic decays to muons. The dominant backgrounds are
evaluated directly from the data. Based on 20 candidate
events and an expected background of 9.5±1.1 events, we
measure a production cross section of 5.3±3.3-1.0+1.3 pb,
in agreement with the standard model. © 2005 The American
Physical Society.},
Doi = {10.1103/PhysRevD.72.032002},
Key = {fds313578}
}
@article{fds308147,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery,
M},
Title = {Measurement of the tt̄ production cross section in pp̄
collisions at √s = 1.96 TeV using lepton + jets events
with secondary vertex b -tagging},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {5},
Pages = {1-28},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.71.052003},
Abstract = {We present a measurement of the tt̄ production cross
section using events with one charged lepton and jets from
pp̄ collisions at a center-of-mass energy of 1.96 TeV. In
these events, heavy flavor quarks from top quark decay are
identified with a secondary vertex tagging algorithm. From
162 pb<sup>-1</sup> of data collected by the Collider
Detector at Fermilab, a total of 48 candidate events are
selected, where 13.5 ± 1.8 events are expected from
background contributions. We measure a tt̄ production cross
section of 5.6<inf>-1.1</inf><sup>+1.2</sup>(stat.)<inf>-0.6</inf><sup>+0.9</sup>(syst.)
pb. © 2005 The American Physical Society.},
Doi = {10.1103/PhysRevD.71.052003},
Key = {fds308147}
}
@article{fds313580,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli,
M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron,
S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen,
C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang,
S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker,
GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, J and Frisch,
H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko,
I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann,
SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefevre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson,
M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel,
P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr,
B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller,
T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu,
C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov,
T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh,
SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn,
F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno,
M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet,
M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba,
A},
Title = {Measurement of the tt̄ production cross section in pp̄
collisions at √s=1:96 TeV using kinematic fitting of
b-tagged lepton+jet events},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {7},
Pages = {1-11},
Publisher = {American Physical Society (APS)},
Year = {2005},
ISSN = {1550-7998},
url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000228765400011&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
Abstract = {We report a measurement of the tt̄ production cross section
using the CDF II detector at the Fermilab Tevatron. The data
consist of events with an energetic electron or muon,
missing transverse energy, and three or more hadronic jets,
at least one of which is identified as a b-quark jet by
reconstructing a secondary vertex. The background fraction
is determined from a fit of the transverse energy of the
leading jet. Using 162 ± 10 pb -1 of data, the total cross
section is found to be 6.0 ± 1.6(stat.) ± 1.2(syst.) pb,
which is consistent with the standard model prediction. ©
2005 The American Physical Society.},
Doi = {10.1103/PhysRevD.71.072005},
Key = {fds313580}
}
@article{fds307991,
Author = {Aaltonen, T and others},
Title = {Measurement of the tt̅ cross section in pp̅ collisions at
sqrt[s] =1.96 TeV using dilepton events with a lepton plus
track selection},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {11},
Pages = {112007},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112007},
Abstract = {This paper reports a measurement of the cross section for
the pair production of top quarks in pp̅ collisions at
sqrt[s]=1.96 TeV at the Fermilab Tevatron. The data
were collected from the CDF run II detector in a set of runs
with a total integrated luminosity of 1.1 fb-1. The
cross section is measured in the dilepton channel, the
subset of tt̅ events in which both top quarks decay through
t→Wb→ℓνb, where ℓ=e, μ, or τ. The lepton pair is
reconstructed as one identified electron or muon and one
isolated track. The use of an isolated track to identify the
second lepton increases the tt̅ acceptance, particularly
for the case in which one W decays as W→τν. The purity
of the sample may be further improved at the cost of a
reduction in the number of signal events, by requiring an
identified b jet. We present the results of measurements
performed with and without the request of an identified b
jet. The former is the first published CDF result for which
a b-jet requirement is added to the dilepton selection. In
the CDF data there are 129 pretag lepton+track candidate
events, of which 69 are tagged. With the tagging
information, the sample is divided into tagged and untagged
subsamples, and a combined cross section is calculated by
maximizing a likelihood. The result is σtt̅ =9.6 ±
1.2(stat)-0.5+0.6(sys) ± 0.6(lum) pb, assuming a
branching ratio of BR(W→ℓν)=10.8% and a top mass of
mt=175 GeV/c2.},
Doi = {10.1103/PhysRevD.79.112007},
Key = {fds307991}
}
@article{fds307982,
Author = {Aaltonen, T and others},
Title = {Measurement of the t[overline t] production cross section in
2 fb[sup -1] of p[overline p] collisions at sqrt(s) = 1.96
TeV using lepton plus jets events with soft muon b
tagging},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {5},
Pages = {052007},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.052007},
Abstract = {We present a measurement of the tt̄ production cross
section in pp̄ collisions at s=1.96TeV using events
containing a high transverse momentum electron or muon,
three or more jets, and missing transverse energy. Events
consistent with tt̄ decay are found by identifying jets
containing candidate heavy-flavor semileptonic decays to
muons. The measurement uses a CDF run II data sample
corresponding to 2fb-1 of integrated luminosity. Based on
248 candidate events with three or more jets and an expected
background of 79.5±5.3 events, we measure a production
cross section of 9.1±1.6pb. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.052007},
Key = {fds307982}
}
@article{fds310368,
Author = {The ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa,
C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung,
C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso,
S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurement of the underlying event in jet events from
7 TeV proton–proton collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {74},
Number = {8},
Pages = {1-29},
Publisher = {Springer Nature},
Year = {2014},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2965-5},
Abstract = {Distributions sensitive to the underlying event in QCD jet
events have been measured with the ATLAS detector at the
LHC, based on (Formula presented.) of proton–proton
collision data collected at a centre-of-mass energy of
7 (Formula presented.). Charged-particle mean (Formula
presented.) and densities of all-particle (Formula
presented.) and charged-particle multiplicity and (Formula
presented.) have been measured in regions azimuthally
transverse to the hardest jet in each event. These are
presented both as one-dimensional distributions and with
their mean values as functions of the leading-jet transverse
momentum from 20 to 800 (Formula presented.). The
correlation of charged-particle mean (Formula presented.)
with charged-particle multiplicity is also studied, and the
(Formula presented.) densities include the forward rapidity
region; these features provide extra data constraints for
Monte Carlo modelling of colour reconnection and
beam-remnant effects respectively. For the first time,
underlying event observables have been computed separately
for inclusive jet and exclusive dijet event selections,
allowing more detailed study of the interplay of multiple
partonic scattering and QCD radiation contributions to the
underlying event. Comparisons to the predictions of
different Monte Carlo models show a need for further model
tuning, but the standard approach is found to generally
reproduce the features of the underlying event in both types
of event selection.},
Doi = {10.1140/epjc/s10052-014-2965-5},
Key = {fds310368}
}
@article{fds307765,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni, G},
Title = {Measurement of the W ±Z production cross section
and limits on anomalous triple gauge couplings in
proton-proton collisions at s=7 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {709},
Number = {4-5},
Pages = {341-357},
Publisher = {Elsevier BV},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2012.02.053},
Abstract = {This Letter presents a measurement of W ±Z production in
1.02 fb -1 of pp collision data at s=7 TeV collected by the
ATLAS experiment in 2011. Doubly leptonic decay events are
selected with electrons, muons and missing transverse
momentum in the final state. In total 71 candidates are
observed, with a background expectation of
12.1±1.4(stat.)-2.0+4.1(syst.) events. The total cross
section for W ±Z production for Z/γ * masses within the
range 66 GeV to 116 GeV is determined to be
σWZtot=20.5-2.8+3.1(stat.)-1.3+1.4(syst.)-0.8+0.9(lumi.)
pb, which is consistent with the Standard Model expectation
of 17.30.8+1.3 pb. Limits on anomalous triple gauge boson
couplings are extracted. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.02.053},
Key = {fds307765}
}
@booklet{Abbott98a,
Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
Alves and N. Amos and E. W. Anderson and R. Astur and M. M.
Baarmand and A. Baden and V. Balamurali and J. Balderston and B. Baldin and},
Title = {Measurement of the W boson mass},
Journal = {Physical Review D},
Volume = {5809},
Number = {9},
Pages = {art. no. -- 092003},
Year = {1998},
Month = {November},
Key = {Abbott98a}
}
@article{fds308238,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Measurement of the W boson mass},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {58},
Number = {9},
Pages = {920031-9200337},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.58.092003},
Abstract = {We present a measurement of the W boson mass using data
collected by the D0 experiment at the Fermilab Tevatron
during 1994–1995. We identify W bosons by their decays to
[Formula Presented] final states. We extract the W mass
[Formula Presented] by fitting the transverse mass and
transverse electron momentum spectra from a sample of 28 323
[Formula Presented] decay candidates. We use a sample of
3563 dielectron events, mostly due to [Formula Presented]
decays, to constrain our model of the detector response.
From the transverse mass fit we measure [Formula Presented]
GeV. Combining this with our previously published result
from data taken in 1992–1993, we obtain [Formula
Presented]. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevD.58.092003},
Key = {fds308238}
}
@article{fds308046,
Author = {Kotwal, AV and Stark, J},
Title = {Measurement of the W boson mass at the Tevatron},
Journal = {Annual Reviews of Nuclear and Particle Science},
Volume = {58},
Number = {1},
Pages = {28},
Publisher = {ANNUAL REVIEWS},
Year = {2008},
Month = {November},
url = {http://dx.doi.org/10.1146/annurev.nucl.58.110707.171227},
Abstract = {Over the past four decades, the standard model of
electroweak interactions has achieved tremendous success in
describing the experimental data. One of the key observables
is the mass M w of the W boson. The experimental
measurements, including M w, have reached a level of
precision that tests the theory at the quantum loop level,
providing indirect constraints on the hypothetical Higgs
boson and other new physics. Improved measurements of M w
are driven by new data from Run II of the Fermilab Tevatron
(pp̄ collider at ̂s = 1.96 TeV). We discuss the techniques
used for measuring M w at hadron colliders, summarize the
measurements from Run I of the Tevatron, and review the
state of the art of the Run II analyses, which are based on
significantly larger data sets collected with upgraded
detectors. We discuss the constraints on the Higgs boson,
and conclude with a discussion of the ultimate precision in
M w that can be expected from Run II. Copyright © 2008 by
Annual Reviews. All rights reserved.},
Doi = {10.1146/annurev.nucl.58.110707.171227},
Key = {fds308046}
}
@article{fds308195,
Author = {Song, XF and Sosebee, M and Sotnikova, N and Souza, M and Stanton, NR and Steinbruck, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink, M and Stutte, L and Sznajder, A and Tamburello, P and Tarazi,
J and Tartaglia, M and Thomas, TL and Thompson, J and Toback, D and Trippe,
TG and Turcot, AS and Tuts, PM},
Title = {Measurement of the W boson mass using electrons at large
rapidities},
Journal = {Physical review letters},
Volume = {84},
Number = {2},
Pages = {222-227},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.84.222},
Abstract = {We report a measurement of the W boson mass based on an
integrated luminosity of 82 pb(-1) from p&pmacr; collisions
at sqrt[s] = 1.8 TeV recorded in 1994-1995 by the D0
detector at the Fermilab Tevatron. We identify W bosons by
their decays to enu, where the electron is detected in the
forward calorimeters. We extract the mass by fitting the
transverse mass and the electron and neutrino transverse
momentum spectra of 11 089 W boson candidates. We measure
M(W) = 80.691+/-0.227 GeV. By combining this measurement
with our previously published central calorimeter results
from data taken in 1992-1993 and 1994-1995, we obtain M(W) =
80.482+/-0.091 GeV.},
Doi = {10.1103/physrevlett.84.222},
Key = {fds308195}
}
@article{fds308198,
Author = {Abbott, B and al, E},
Title = {Measurement of the W boson mass using large rapidity
electrons},
Journal = {Phys. Rev. D},
Volume = {62},
Number = {092006},
Pages = {33},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.62.092006},
Abstract = {We present a measurement of the W boson mass using data
collected by the DØ experiment at the Fermilab Tevatron
during 1994-1995. We identify W bosons by their decays to
enu final states where the electron is detected in a forward
calorimeter. We extract the W boson mass MW by fitting the
transverse mass and transverse electron and neutrino
momentum spectra from a sample of 11089 W->enu decay
candidates. We use a sample of 1687 dielectron events,
mostly due to Z->ee decays, to constrain our model of the
detector response. Using the forward calorimeter data, we
measure MW = 80.691±0.227 GeV.},
Doi = {10.1103/PhysRevD.62.092006},
Key = {fds308198}
}
@article{fds307783,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A},
Title = {Measurement of the W boson polarization in top quark decays
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {6},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2012)088},
Abstract = {This paper presents measurements of the polarization ofW
bosons in top quark decays, derived from tt̄ events with
missing transverse momentum, one charged lepton and at least
four jets, or two charged leptons and at least two jets.
Data from pp collisions at a centre-of-mass energy of 7 TeV
were collected with the ATLAS experiment at the LHC and
correspond to an integrated luminosity of 1.04 fb-1. The
measured fractions of longitudinally, left- and right-handed
polarization are F0 = 0.67 ± 0.07, FL = 0.32 ± 0.04 and FR
= 0.01 ± 0.05, in agreement with the Standard Model
predictions. As the polarization of the W bosons in top
quark decays is sensitive to the Wtb vertex Lorentz
structure and couplings, the measurements were used to set
limits on anomalous contributions to the Wtb couplings. ©
CERN.},
Doi = {10.1007/JHEP06(2012)088},
Key = {fds307783}
}
@article{fds313618,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurement of the W W + W Z cross section and limits on
anomalous triple gauge couplings using final states with one
lepton, missing transverse momentum, and two jets with the
ATLAS detector at √s = 7 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {1},
Pages = {1-42},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2015)049},
Abstract = {Abstract: The production of a W boson decaying to eν or
μν in association with a W or Z boson decaying to two jets
is studied using 4.6 fb−1 of proton-proton collision data
at √s =7 TeV recorded with the ATLAS detector at the LHC.
The combined WW + WZ cross section is measured with a
significance of 3.4σ and is found to be 68±7 (stat.)±19
(syst.) pb, in agreement with the Standard Model expectation
of 61.1±2.2 pb. The distribution of the transverse momentum
of the dijet system is used to set limits on anomalous
contributions to the triple gauge coupling vertices and on
parameters of an effective-field-theory model.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP01(2015)049},
Key = {fds313618}
}
@article{fds307842,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Baltasar Dos Santos Pedrosa,
F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates,
RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
M and Benedict, BH and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci,
F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Biesiada, J and Biglietti,
M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Boonekamp, M and Boorman,
G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boulahouache, C and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Brubaker, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse,
M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camard,
A and Camarri, P and Cambiaghi, M and Cameron, D and Cammin, J and Campana,
S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Cazzato, A and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, L and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov,
A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Measurement of the W+ W- cross section in sqrt(s) =
7 TeV pp collisions with ATLAS.},
Journal = {Physical review letters},
Volume = {107},
Number = {4},
Pages = {041802},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.107.041802},
Abstract = {This Letter presents a measurement of the W+ W- production
cross section in sqrt(s) = 7 TeV pp collisions by the
ATLAS experiment, using 34 pb(-1) of integrated
luminosity produced by the Large Hadron Collider at CERN.
Selecting events with two isolated leptons, each either an
electron or a muon, 8 candidate events are observed with an
expected background of 1.7 ± 0.6 events. The measured cross
section is 41(-16)(+20)(stat) ± 5(syst)±1(lumi) pb,
which is consistent with the standard model prediction of 44
± 3 pb calculated at next-to-leading order in
QCD.},
Doi = {10.1103/physrevlett.107.041802},
Key = {fds307842}
}
@article{fds356730,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of the W+W− production
cross section in pp collisions at a centre-of-mass energy of
√s = 13 TeV with the ATLAS experiments},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {773},
Pages = {354-374},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2017.08.047},
Abstract = {The production of opposite-charge W-boson pairs in
proton–proton collisions at s=13 TeV is measured using
data corresponding to 3.16 fb−1 of integrated luminosity
collected by the ATLAS detector at the CERN Large Hadron
Collider in 2015. Candidate W-boson pairs are selected by
identifying their leptonic decays into an electron, a muon
and neutrinos. Events with reconstructed jets are not
included in the candidate event sample. The cross-section
measurement is performed in a fiducial phase space close to
the experimental acceptance and is compared to theoretical
predictions. Agreement is found between the measurement and
the most accurate calculations available.},
Doi = {10.1016/j.physletb.2017.08.047},
Key = {fds356730}
}
@article{fds321134,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of the W±Z boson pair-production
cross section in pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {762},
Pages = {1-22},
Publisher = {Elsevier BV},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.052},
Abstract = {The production of W±Z events in proton–proton collisions
at a centre-of-mass energy of 13 TeV is measured with the
ATLAS detector at the LHC. The collected data correspond to
an integrated luminosity of 3.2 fb−1. The W±Z candidates
are reconstructed using leptonic decays of the gauge bosons
into electrons or muons. The measured inclusive cross
section in the detector fiducial region for leptonic decay
modes is σW±Z→ℓ′νℓℓfid.=63.2±3.2(stat.)±2.6(sys.)±1.5(lumi.)
fb. In comparison, the next-to-leading-order Standard Model
prediction is 53.4−2.8+3.6 fb. The extrapolation of the
measurement from the fiducial to the total phase space
yields σW±Ztot.=50.6±2.6(stat.)±2.0(sys.)±0.9(th.)±1.2(lumi.)
pb, in agreement with a recent next-to-next-to-leading-order
calculation of 48.2−1.0+1.1 pb. The cross section as a
function of jet multiplicity is also measured, together with
the charge-dependent W+Z and W−Z cross sections and their
ratio.},
Doi = {10.1016/j.physletb.2016.08.052},
Key = {fds321134}
}
@article{fds321103,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Measurement of the WW and WZ production cross section using
final states with a charged lepton and heavy-flavor jets in
the full CDF Run II data set},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032008},
Abstract = {We present a measurement of the total WW and WZ production
cross sections in pp collision at s=1.96 TeV, in a final
state consistent with leptonic W boson decay and jets
originating from heavy-flavor quarks from either a W or a Z
boson decay. This analysis uses the full data set collected
with the CDF II detector during Run II of the Tevatron
collider, corresponding to an integrated luminosity of 9.4
fb-1. An analysis of the dijet mass spectrum provides 3.7σ
evidence of the summed production processes of either WW or
WZ bosons with a measured total cross section of
σWW+WZ=13.7±3.9 pb. Independent measurements of the WW and
WZ production cross sections are allowed by the different
heavy-flavor decay patterns of the W and Z bosons and by the
analysis of secondary-decay vertices reconstructed within
heavy-flavor jets. The productions of WW and of WZ dibosons
are independently seen with significances of 2.9σ and
2.1σ, respectively, with total cross sections of
σWW=9.4±4.2 pb and σWZ=3.7-2.2+2.5 pb. The measurements
are consistent with standard-model predictions.},
Doi = {10.1103/PhysRevD.94.032008},
Key = {fds321103}
}
@article{fds307780,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC},
Title = {Measurement of the WW cross section in √s=7 TeV pp
collisions with the ATLAS detector and limits on anomalous
gauge couplings},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {712},
Number = {4-5},
Pages = {289-308},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.05.003},
Abstract = {This Letter reports a measurement of the WW production cross
section in √s=7 TeV pp collisions using data corresponding
to an integrated luminosity of 1.02 fb-1 collected with the
ATLAS detector. Using leptonic decays of oppositely charged
W bosons, the total measured cross section is
σ(pp→WW)=54.4±4.0(stat.)±3.9(syst.)±2.0(lumi.) pb,
consistent with the Standard Model prediction of
σ(pp→WW)=44.4±2.8 pb. Limits on anomalous electroweak
triple-gauge couplings are extracted from a fit to the
transverse-momentum distribution of the leading charged
lepton in the event. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.05.003},
Key = {fds307780}
}
@article{fds307810,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Measurement of the WZ cross section and triple gauge
couplings in pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.031104},
Abstract = {This article describes the current most precise measurement
of the WZ production cross section as well as limits on
anomalous WWZ couplings at a center-of-mass energy of 1.96
TeV in proton-antiproton collisions for the Collider
Detector at Fermilab (CDF). WZ candidates are reconstructed
from decays containing three charged leptons and missing
energy from a neutrino, where the charged leptons are either
electrons or muons. Using data collected by the CDF II
detector (7.1fb -1 of integrated luminosity), 63 candidate
events are observed with the expected background
contributing 8±1 events. The measured total cross section
σ(pp̄→WZ)=3.93-0.53+0.60(stat)-0. 46+0.59(syst)pb is in
good agreement with the standard model prediction of
3.50±0.21. The same sample is used to set limits on
anomalous WWZ couplings. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.031104},
Key = {fds307810}
}
@article{fds307751,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Measurement of the W→τντ cross section in pp
collisions at s=7 TeV with the ATLAS experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {706},
Number = {4-5},
Pages = {276-294},
Publisher = {Elsevier BV},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2011.11.057},
Abstract = {The cross section for the production of W bosons with
subsequent decay W→τντ is measured with the ATLAS
detector at the LHC. The analysis is based on a data sample
that was recorded in 2010 at a proton-proton center-of-mass
energy of s=7 TeV and corresponds to an integrated
luminosity of 34 pb-1. The cross section is measured in a
region of high detector acceptance and then extrapolated to
the full phase space. The product of the total W production
cross section and the W→τντ branching ratio is measured
to be σW→τντtot=11.1±0.3(stat)±1.7(syst)±0.4(lumi)
nb. © 2011 CERN.},
Doi = {10.1016/j.physletb.2011.11.057},
Key = {fds307751}
}
@article{fds356538,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Measurement of the Z(→ ℓ + ℓ
−)γ production cross-section in pp collisions at
√s = 13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {3},
Year = {2020},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2020)054},
Abstract = {The production of a prompt photon in association with a Z
boson is studied in proton-proton collisions at a
centre-of-mass energy s = 13 TeV. The analysis uses a data
sample with an integrated luminosity of 139 fb−1 collected
by the ATLAS detector at the LHC from 2015 to 2018. The
production cross-section for the process pp → ℓ+ℓ−γ
+ X (ℓ = e, μ) is measured within a fiducial phase-space
region defined by kinematic requirements on the photon and
the leptons, and by isolation requirements on the photon. An
experimental precision of 2.9% is achieved for the fiducial
cross-section. Differential cross-sections are measured as a
function of each of six kinematic variables characterising
the ℓ+ℓ−γ system. The data are compared with
theoretical predictions based on next-to-leading-order and
next-to-next-to-leading-order perturbative QCD calculations.
The impact of next-to-leading-order electroweak corrections
is also considered. [Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP03(2020)054},
Key = {fds356538}
}
@article{fds317301,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurement of the Z/γ* boson transverse
momentum distribution in pp collisions at √s = 7 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Publisher = {Springer Nature},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2014)145},
Abstract = {This paper describes a measurement of the Z/γ* boson
transverse momentum spectrum using ATLAS proton-proton
collision data at a centre-of-mass energy of (Formula
presented) TeV at the LHC. The measurement is performed in
the Z/γ* → e+e− and Z/γ* → μ+μ− channels, using
data corresponding to an integrated luminosity of 4.7
fb−1. Normalized differential cross sections as a function
of the Z/γ* boson transverse momentum are measured for
transverse momenta up to 800 GeV. The measurement is
performed inclusively for Z/γ* rapidities up to 2.4, as
well as in three rapidity bins. The channel results are
combined, compared to perturbative and resummed QCD
calculations and used to constrain the parton shower
parameters of Monte Carlo generators.},
Doi = {10.1007/JHEP09(2014)145},
Key = {fds317301}
}
@article{fds307714,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten,
K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benjamin,
DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius,
C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan,
JG and Coggeshall, J and Cogneras, E and Cojocaru,
CD},
Title = {Measurement of the ZZ production cross section and limits on
anomalous neutral triple gauge couplings in proton-proton
collisions at sqrt[s] = 7 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {108},
Number = {4},
Pages = {041804},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.108.041804},
Abstract = {A measurement of the ZZ production cross section in
proton-proton collisions at sqrt[s] = 7 TeV using data
corresponding to an integrated luminosity of 1.02 fb(-1)
recorded by the ATLAS experiment at the LHC is presented.
Twelve events containing two Z boson candidates decaying to
electrons and/or muons are observed, with an expected
background of 0.3 ± 0.3(stat)(-0.3)(+0.4)(syst) events. The
cross section measured in a phase-space region with good
detector acceptance and for dilepton masses within the range
66 to 116 GeV is σ(ZZ → ℓ+ ℓ- ℓ+ ℓ-)(fid) =
19.4(-5.2)(+6.3)(stat)(-0.7)(+0.9)(syst) ± 0.7(lumi) fb.
The resulting total cross section for on-shell ZZ
production, σ(ZZ)(tot) = 8.5(-2.3)(+2.7)(stat)(-0.3)(+0.4)(syst)
± 0.3(lumi) pb, is consistent with the standard model
expectation of 6.5(-0.2)(+0.3) pb calculated at the
next-to-leading order in QCD. Limits on anomalous neutral
triple gauge boson couplings are derived.},
Doi = {10.1103/physrevlett.108.041804},
Key = {fds307714}
}
@article{fds347513,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram,
IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia
Bylund, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa,
A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chouridou,
S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou,
Y},
Title = {Measurement of the ZZ Production Cross Section in pp
Collisions at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {116},
Number = {10},
Pages = {101801},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.116.101801},
Abstract = {The ZZ production cross section in proton-proton collisions
at 13 TeV center-of-mass energy is measured using
3.2 fb^{-1} of data recorded with the ATLAS detector at
the Large Hadron Collider. The considered Z boson candidates
decay to an electron or muon pair of mass 66-116 GeV. The
cross section is measured in a fiducial phase space
reflecting the detector acceptance. It is also extrapolated
to a total phase space for Z bosons in the same mass range
and of all decay modes, giving 16.7_{-2.0}^{+2.2}(stat)+0.9/-0.7(syst)+1.0/-0.7(lumi) pb.
The results agree with standard model predictions.},
Doi = {10.1103/physrevlett.116.101801},
Key = {fds347513}
}
@article{fds356766,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Measurement of the ZZ production cross section in
proton-proton collisions at √s=8 TeV using the ZZ →
ℓ−ℓ+ℓ′−ℓ′+
and ZZ→ ℓ−ℓ+νν¯ decay
channels with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {1},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2017)099},
Abstract = {A measurement of the ZZ production cross section in the
ℓ−ℓ+ℓ′ −ℓ′ + and ℓ−ℓ+νν¯ channels
(ℓ = e, μ) in proton-proton collisions at s=8TeV at the
Large Hadron Collider at CERN, using data corresponding to
an integrated luminosity of 20.3 fb−1 collected by the
ATLAS experiment in 2012 is presented. The fiducial cross
sections for ZZ → ℓ−ℓ+ℓ′ −ℓ′ + and ZZ→
ℓ−ℓ+νν¯ are measured in selected phase-space
regions. The total cross section for ZZ events produced with
both Z bosons in the mass range 66 to 116 GeV is measured
from the combination of the two channels to be 7.3 ±
0.4(stat) ± 0.3(syst)− 0.1− 0.2(lumi) pb, which is
consistent with the Standard Model prediction of 6. 6−
0.6+ 0.7 pb. The differential cross sections in bins of
various kinematic variables are presented. The differential
event yield as a function of the transverse momentum of the
leading Z boson is used to set limits on anomalous neutral
triple gauge boson couplings in ZZ production.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP01(2017)099},
Key = {fds356766}
}
@article{fds310379,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Measurement of the ZZ production cross section using the
full CDF II data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.89.112001},
Abstract = {We present a measurement of the ZZ-boson pair-production
cross section in 1.96 TeV center-of-mass energy pp̄
collisions. We reconstruct final states incorporating four
charged leptons or two charged leptons and two neutrinos
from the full data set collected by the Collider Detector
experiment at the Fermilab Tevatron, corresponding to
9.7fb-1 of integrated luminosity. Combining the results
obtained from each final state, we measure a cross section
of 1.04-0.25+0.32pb, in good agreement with the standard
model prediction at next-to-leading order in the
strong-interaction coupling. © 2014 American Physical
Society.},
Doi = {10.1103/PhysRevD.89.112001},
Key = {fds310379}
}
@article{fds347453,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Measurement of the Zγ→ νν¯ γ production cross section
in pp collisions at √s=13 TeV with the ATLAS detector and
limits on anomalous triple gauge-boson couplings},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {12},
Year = {2018},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2018)010},
Abstract = {The production of Z bosons in association with a high-energy
photon (Zγ production) is studied in the neutrino decay
channel of the Z boson using pp collisions at s=13 TeV. The
analysis uses a data sample with an integrated luminosity of
36.1fb−1 collected by the ATLAS detector at the LHC in
2015 and 2016. Candidate Zγ events with invisible decays of
the Z boson are selected by requiring significant transverse
momentum (pT) of the dineutrino system in conjunction with a
single isolated photon with large transverse energy (ET).
The rate of Zγ production is measured as a function of
photon ET, dineutrino system pT and jet multiplicity.
Evidence of anomalous triple gauge-boson couplings is sought
in Zγ production with photon ET greater than 600 GeV. No
excess is observed relative to the Standard Model
expectation, and upper limits are set on the strength of
ZZγ and Zγγ couplings.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP12(2018)010},
Key = {fds347453}
}
@article{fds307854,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Measurement of the Z→ττ cross section with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {84},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.84.112006},
Abstract = {The Z→ττ cross section is measured with the ATLAS
experiment at the LHC in four different final states
determined by the decay modes of the τ leptons:
muon-hadron, electron-hadron, electron-muon, and muon-muon.
The analysis is based on a data sample corresponding to an
integrated luminosity of 36pb-1, at a proton-proton
center-of-mass energy of √s=7TeV. Cross sections are
measured separately for each final state in fiducial regions
of high detector acceptance, as well as in the full phase
space, over the mass region 66-116 GeV. The individual cross
sections are combined and the product of the total Z
production cross section and Z→ττ branching fraction is
measured to be 0.97±0.07(stat)±0.06(syst)±0.03(lumi)nb,
in agreement with next-to-next-to-leading order
calculations. © 2011 CERN.},
Doi = {10.1103/PhysRevD.84.112006},
Key = {fds307854}
}
@article{fds347489,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett,
RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr,
AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone,
RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli,
A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
MR},
Title = {Measurement of the [Formula: see text] and [Formula: see
text] production cross sections in multilepton final states
using 3.2 fb[Formula: see text] of [Formula: see text]
collisions at [Formula: see text] = 13 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {1},
Pages = {40},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4574-y},
Abstract = {A measurement of the [Formula: see text] and [Formula: see
text] production cross sections in final states with either
two same-charge muons, or three or four leptons (electrons
or muons) is presented. The analysis uses a data sample of
proton-proton collisions at [Formula: see text] TeV recorded
with the ATLAS detector at the Large Hadron Collider in
2015, corresponding to a total integrated luminosity of
3.2 fb[Formula: see text]. The inclusive cross sections are
extracted using likelihood fits to signal and control
regions, resulting in [Formula: see text] pb and [Formula:
see text] pb, in agreement with the Standard Model
predictions.},
Doi = {10.1140/epjc/s10052-016-4574-y},
Key = {fds347489}
}
@article{fds322001,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez,
VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Measurement of the [Formula: see text] dijet cross section
in pp collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {12},
Pages = {670},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4521-y},
Abstract = {The dijet production cross section for jets containing a
b-hadron (b-jets) has been measured in proton-proton
collisions with a centre-of-mass energy of [Formula: see
text] TeV, using the ATLAS detector at the LHC. The data
used correspond to an integrated luminosity of [Formula: see
text]. The cross section is measured for events with two
identified b-jets with a transverse momentum [Formula: see
text] GeV and a minimum separation in the [Formula: see
text]-[Formula: see text] plane of [Formula: see text]. At
least one of the jets in the event is required to have
[Formula: see text] GeV. The cross section is measured
differentially as a function of dijet invariant mass, dijet
transverse momentum, boost of the dijet system, and the
rapidity difference, azimuthal angle and angular distance
between the b-jets. The results are compared to different
predictions of leading order and next-to-leading order
perturbative quantum chromodynamics matrix elements
supplemented with models for parton-showers and
hadronization.},
Doi = {10.1140/epjc/s10052-016-4521-y},
Key = {fds322001}
}
@article{fds307616,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio,
EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas,
CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
Title = {Measurement of the [Formula: see text] production cross
section in the tau + jets channel using the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {3},
Pages = {2328},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2328-7},
Abstract = {A measurement of the top quark pair production cross section
in the final state with a hadronically decaying tau lepton
and jets is presented. The analysis is based on
proton-proton collision data recorded by the ATLAS
experiment at the LHC, with a centre-of-mass energy of
7 TeV. The data sample corresponds to an integrated
luminosity of 1.67 fb<sup>-1</sup>. The cross section is
measured to be [Formula: see text] and is in agreement with
other measurements and with the Standard Model
prediction.},
Doi = {10.1140/epjc/s10052-013-2328-7},
Key = {fds307616}
}
@article{fds310393,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, MF and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Measurement of the [Formula: see text] production
cross-section using [Formula: see text] events with
[Formula: see text]-tagged jets in [Formula: see text]
collisions at [Formula: see text] and 8 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {10},
Pages = {3109},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3109-7},
Abstract = {The inclusive top quark pair ([Formula: see text])
production cross-section [Formula: see text] has been
measured in proton-proton collisions at [Formula: see text]
and [Formula: see text] with the ATLAS experiment at the
LHC, using [Formula: see text] events with an
opposite-charge [Formula: see text] pair in the final state.
The measurement was performed with the 2011 7 TeV dataset
corresponding to an integrated luminosity of 4.6 [Formula:
see text] and the 2012 8 TeV dataset of 20.3 [Formula: see
text]. The numbers of events with exactly one and exactly
two [Formula: see text]-tagged jets were counted and used to
simultaneously determine [Formula: see text] and the
efficiency to reconstruct and [Formula: see text]-tag a jet
from a top quark decay, thereby minimising the associated
systematic uncertainties. The cross-section was measured to
be: [Formula: see text]where the four uncertainties arise
from data statistics, experimental and theoretical
systematic effects, knowledge of the integrated luminosity
and of the LHC beam energy. The results are consistent with
recent theoretical QCD calculations at next-to-next-to-leading
order. Fiducial measurements corresponding to the
experimental acceptance of the leptons are also reported,
together with the ratio of cross-sections measured at the
two centre-of-mass energies. The inclusive cross-section
results were used to determine the top quark pole mass via
the dependence of the theoretically predicted cross-section
on [Formula: see text] giving a result of [Formula: see
text][Formula: see text] GeV. By looking for an excess of
[Formula: see text] production with respect to the QCD
prediction, the results were also used to place limits on
the pair-production of supersymmetric top squarks [Formula:
see text] with masses close to the top quark mass, decaying
via [Formula: see text] to predominantly right-handed top
quarks and a light neutralino [Formula: see text], the
lightest supersymmetric particle. Top squarks with masses
between the top quark mass and 177 GeV are excluded at the
95 % confidence level.},
Doi = {10.1140/epjc/s10052-014-3109-7},
Key = {fds310393}
}
@article{fds307629,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurement of the Λb0 lifetime and mass in the ATLAS
experiment},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.87.032002},
Abstract = {A measurement of the Λb0 lifetime and mass in the decay
channel Λb0→J/ψ(μ+μ-)Λ0(pπ -) is presented. The
analysis uses a signal sample of about 2200 Λb0 and Λ̄b0
decays that are reconstructed in 4.9 fb -1 of ATLAS pp
collision data collected in 2011 at the LHC center-of-mass
energy of 7 TeV. A simultaneous mass and decay time maximum
likelihood fit is used to extract the Λb0 lifetime and
mass. They are measured to be τΛb=1.449±0.036(stat)
±0.017(syst) ps and mΛb=5619.7±0. 7(stat)±1.1(syst)
MeV.},
Doi = {10.1103/PhysRevD.87.032002},
Key = {fds307629}
}
@article{fds344670,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carrillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully,
JC and Cyr, D and Daronco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng,
J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube,
S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell, JL and Ginsburg,
C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute,
M and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Labarga, L and Lai, S and Lami, S and Lammel,
S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
J and Nagano, A and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prokoshin, F and Pronko, A and Proudfoot, J and Ptochos, F and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic,
V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti,
A},
Title = {Measurement of the Λb0 Lifetime in Λb0→J/ψΛ0 in pp̄
Collisions at s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {98},
Number = {12},
Pages = {122001},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevLett.98.122001},
Abstract = {We report a measurement of the Λb0 lifetime in the
exclusive decay Λb0→J/ψΛ0 in pp̄ collisions at
s=1.96TeV using an integrated luminosity of 1.0fb-1 of data
collected by the CDF II detector at the Fermilab Tevatron.
Using fully reconstructed decays, we measure
τ(Λb0)=1.593-0.078+0.083(stat)±0.033(syst)ps. This is the
single most precise measurement of τ(Λb0) and is 3.2σ
higher than the current world average. © 2007 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.98.122001},
Key = {fds344670}
}
@article{fds307864,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
R and Ask, S},
Title = {Measurement of the Υ(1S) production cross-section in pp
collisions at s=7 TeV in ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {705},
Number = {1-2},
Pages = {9-27},
Publisher = {Elsevier BV},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2011.09.092},
Abstract = {A measurement of the cross-section for Υ(1S)→μ+μ-
production in proton-proton collisions at centre of mass
energy of 7 TeV is presented. The cross-section is measured
as a function of the Υ(1S) transverse momentum in two bins
of rapidity, |yΥ(1S)|<1.2 and 1.2<|yΥ(1S)|<2.4. The
measurement requires that both muons have transverse
momentum pTμ>4 GeV and pseudorapidity |ημ|<2.5 in order
to reduce theoretical uncertainties on the acceptance, which
depend on the poorly known polarisation. The results are
based on an integrated luminosity of 1.13 pb-1, collected
with the ATLAS detector at the Large Hadron Collider. The
cross-section measurement is compared to theoretical
predictions: it agrees to within a factor of two with a
prediction based on the NRQCD model including colour-singlet
and colour-octet matrix elements as implemented in Pythia
while it disagrees by up to a factor of ten with the
next-to-leading order prediction based on the colour-singlet
model. © 2011 CERN.},
Doi = {10.1016/j.physletb.2011.09.092},
Key = {fds307864}
}
@article{fds310322,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Measurement of three-jet production cross-sections in
[Formula: see text] collisions at 7 [Formula: see text]
centre-of-mass energy using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {228},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3363-3},
Abstract = {Double-differential three-jet production cross-sections are
measured in proton-proton collisions at a centre-of-mass
energy of [Formula: see text] using the ATLAS detector at
the large hadron collider. The measurements are presented as
a function of the three-jet mass [Formula: see text], in
bins of the sum of the absolute rapidity separations between
the three leading jets [Formula: see text]. Invariant masses
extending up to 5 TeV are reached for [Formula: see
text]. These measurements use a sample of data recorded
using the ATLAS detector in 2011, which corresponds to an
integrated luminosity of [Formula: see text]. Jets are
identified using the anti-[Formula: see text] algorithm with
two different jet radius parameters, [Formula: see text] and
[Formula: see text]. The dominant uncertainty in these
measurements comes from the jet energy scale.
Next-to-leading-order QCD calculations corrected to account
for non-perturbative effects are compared to the
measurements. Good agreement is found between the data and
the theoretical predictions based on most of the available
sets of parton distribution functions, over the full
kinematic range, covering almost seven orders of magnitude
in the measured cross-section values.},
Doi = {10.1140/epjc/s10052-015-3363-3},
Key = {fds310322}
}
@article{fds321077,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of top quark pair differential cross sections in
the dilepton channel in pp collisions at √s =7 and 8 TeV
with ATLAS},
Journal = {Physical Review D},
Volume = {94},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.94.092003},
Abstract = {Measurements of normalized differential cross sections of
top quark pair (tt production are presented as a function of
the mass, the transverse momentum and the rapidity of the tt
system in proton-proton collisions at center-of-mass
energies of s=7 and 8 TeV. The data set corresponds to an
integrated luminosity of 4.6 fb-1 at 7 TeV and 20.2 fb-1 at
8 TeV, recorded with the ATLAS detector at the Large Hadron
Collider. Events with top quark pair signatures are selected
in the dilepton final state, requiring exactly two charged
leptons and at least two jets with at least one of the jets
identified as likely to contain a b hadron. The measured
distributions are corrected for detector effects and
selection efficiency to cross sections at the parton level.
The differential cross sections are compared with different
Monte Carlo generators and theoretical calculations of tt
production. The results are consistent with the majority of
predictions in a wide kinematic range.},
Doi = {10.1103/PhysRevD.94.092003},
Key = {fds321077}
}
@article{fds307557,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arslan, O and Artamonov,
A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith,
L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay,
NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach,
AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek,
P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buehrer, F and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
Title = {Measurement of top quark polarization in top-antitop events
from proton-proton collisions at √s=7 TeV using the
ATLAS detector.},
Journal = {Physical review letters},
Volume = {111},
Number = {23},
Pages = {232002},
Year = {2013},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.111.232002},
Abstract = {This Letter presents measurements of the polarization of the
top quark in top-antitop quark pair events, using
4.7 fb(-1) of proton-proton collision data recorded
with the ATLAS detector at the Large Hadron Collider at
√s=7 TeV. Final states containing one or two isolated
leptons (electrons or muons) and jets are considered. Two
measurements of α(ℓ)P, the product of the leptonic
spin-analyzing power and the top quark polarization, are
performed assuming that the polarization is introduced by
either a CP conserving or a maximally CP violating
production process. The measurements obtained,
α(ℓ)P(CPC)=-0.035±0.014(stat)±0.037(syst) and
α(ℓ)P(CPV)=0.020±0.016(stat)(-0.017)(+0.013)(syst), are
in good agreement with the standard model prediction of
negligible top quark polarization.},
Doi = {10.1103/physrevlett.111.232002},
Key = {fds307557}
}
@article{fds321092,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Measurement of total and differential W + W
− production cross sections in proton-proton
collisions at √s=8 TeV with the ATLAS detector and limits
on anomalous triple-gauge-boson couplings},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)029},
Abstract = {The production of W boson pairs in proton-proton collisions
at s=8 TeV is studied using data corresponding to 20.3
fb−1 of integrated luminosity collected by the ATLAS
detector during 2012 at the CERN Large Hadron Collider. The
W bosons are reconstructed using their leptonic decays into
electrons or muons and neutrinos. Events with reconstructed
jets are not included in the candidate event sample. A total
of 6636 WW candidate events are observed. Measurements are
performed in fiducial regions closely approximating the
detector acceptance. The integrated measurement is corrected
for all acceptance effects and for the W branching fractions
to leptons in order to obtain the total WW production cross
section, which is found to be 71.1 ± 1.1(stat) − 5.0+
5.7(syst) ± 1.4(lumi) pb. This agrees with the
next-to-next-to-leading-order Standard Model prediction of
63. 2− 1.4+ 1.6(scale) ± 1.2(PDF) pb. Fiducial
differential cross sections are measured as a function of
each of six kinematic variables. The distribution of the
transverse momentum of the leading lepton is used to set
limits on anomalous triple-gauge-boson couplings.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP09(2016)029},
Key = {fds321092}
}
@article{fds321135,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åesson, TPA and Akimov, AV and Alberghi,
GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and varez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurement of transverse energy-energy correlations in
multi-jet events in pp collisions at s=7 TeV using the ATLAS
detector and determination of the strong coupling constant
as(mZ)},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {750},
Pages = {427-447},
Publisher = {Elsevier BV},
Year = {2015},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2015.09.050},
Abstract = {High transverse momentum jets produced in pp collisions at a
centre of mass energy of 7 TeV are used to measure the
transverse energy-energy correlation function and its
associated azimuthal asymmetry. The data were recorded with
the ATLAS detector at the LHC in the year 2011 and
correspond to an integrated luminosity of 158 pb-1. The
selection criteria demand the average transverse momentum of
the two leading jets in an event to be larger than 250 GeV.
The data at detector level are well described by Monte Carlo
event generators. They are unfolded to the particle level
and compared with theoretical calculations at
next-to-leading-order accuracy. The agreement between data
and theory is good and provides a precision test of
perturbative Quantum Chromodynamics at large momentum
transfers. From this comparison, the strong coupling
constant given at the Z boson mass is determined to be
as(mZ)=0.1173±0.0010 (exp.) -0.0026+0.0065
(theo.).},
Doi = {10.1016/j.physletb.2015.09.050},
Key = {fds321135}
}
@article{fds307614,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurement of upsilon production in 7 TeV pp collisions at
ATLAS},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.87.052004},
Abstract = {Using 1.8 fb-1 of pp collisions at a center-of-mass energy
of 7 TeV recorded by the ATLAS detector at the Large Hadron
Collider, we present measurements of the production cross
sections of Υ(1S,2S,3S) mesons. Υ mesons are reconstructed
using the dimuon decay mode. Total production cross sections
for pT<70 GeV and in the rapidity interval |yΥ|<2.25 are
measured to be, 8.01±0.02±0.36±0.31 nb,
2.05±0.01±0.12±0.08 nb, and 0.92±0.01±0. 07±0.04 nb,
respectively, with uncertainties separated into statistical,
systematic, and luminosity measurement effects. In addition,
differential cross section times dimuon branching fractions
for Υ(1S), Υ(2S), and Υ(3S) as a function of Υ
transverse momentum pT and rapidity are presented. These
cross sections are obtained assuming unpolarized production.
If the production polarization is fully transverse or
longitudinal with no azimuthal dependence in the helicity
frame, the cross section may vary by approximately ±20%. If
a nontrivial azimuthal dependence is considered, integrated
cross sections may be significantly enhanced by a factor of
2 or more. We compare our results to several theoretical
models of Υ meson production, finding that none provide an
accurate description of our data over the full range of Υ
transverse momenta accessible with this data
set.},
Doi = {10.1103/PhysRevD.87.052004},
Key = {fds307614}
}
@article{fds314800,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Measurement of vector boson plus D∗ (2010)+ meson
production in p-p collisions at s =1.96 TeV MEASUREMENT of
VECTOR BOSON PLUS D∗ (2010)+ ... T. AALTONEN et
al.},
Journal = {Physical Review D},
Volume = {93},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {March},
ISSN = {2470-0010},
url = {http://dx.doi.org/10.1103/PhysRevD.93.052012},
Abstract = {A measurement of vector boson (V) production in conjunction
with a D∗(2010)+ meson is presented. Using a data sample
corresponding to 9.7 fb-1 of proton-antiproton collisions at
center-of-mass energy s=1.96 TeV produced by the Fermilab
Tevatron, we reconstruct V+D∗+ samples with the CDF II
detector. The D∗+ is fully reconstructed in the
D∗(2010)+→D0(→K-π+)π+ decay mode. This technique is
sensitive to the associated production of vector boson plus
charm or bottom mesons. We measure the ratio of production
cross sections σ(W+D∗)/σ(W)=[1.75±0.13(stat)±0.09(stat)]%
and σ(Z+D∗)/σ(Z)=[1.5±0.4(stat)±0.2(stat)]% and
perform a differential measurement of dσ(W+D∗)/dpT(D∗).
Event properties are utilized to determine the fraction of
V+D∗(2010)+ events originating from different production
processes. The results are in agreement with the predictions
obtained with the pythia program, limiting possible
contribution from non-standard-model physics
processes.},
Doi = {10.1103/PhysRevD.93.052012},
Key = {fds314800}
}
@article{fds356604,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V},
Title = {Measurement of VH, H → b b ¯ production as a function of
the vector-boson transverse momentum in 13 TeV pp collisions
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2019)141},
Abstract = {Cross-sections of associated production of a Higgs boson
decaying into bottomquark pairs and an electroweak gauge
boson, W or Z, decaying into leptons are measured as a
function of the gauge boson transverse momentum. The
measurements are performed in kinematic fiducial volumes
defined in the ‘simplified template cross-section’
framework. The results are obtained using 79.8 fb−1 of
proton-proton collisions recorded by the ATLAS detector at
the Large Hadron Collider at a centre-of-mass energy of 13
TeV. All measurements are found to be in agreement with the
Standard Model predictions, and limits are set on the
parameters of an effective Lagrangian sensitive to
modifications of the Higgs boson couplings to the
electroweak gauge bosons.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP05(2019)141},
Key = {fds356604}
}
@article{fds308225,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison,
J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher,
S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE and Fortner, M and Frame, KC},
Title = {Measurement of W and Z boson production cross sections in
[formula presented] collisions at [formula presented]
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {5},
Pages = {1-21},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.60.052003},
Abstract = {DØhas measured the inclusive production cross section of W
and Z bosons in a sample of 13 (Formula presented) of data
collected at the Fermilab Tevatron. The cross sections,
multiplied by their leptonic branching fractions, for
production in (Formula presented) collisions at (Formula
presented) TeV are (Formula presented) (Formula presented)
(Formula presented), and (Formula presented), where the
first uncertainty is statistical and the second systematic;
the third reflects the uncertainty in the integrated
luminosity. For the combined electron and muon analyses, we
find (Formula presented). Assuming standard model couplings,
we use this result to determine the width of the W boson,
and obtain (Formula presented). © 1999 The American
Physical Society.},
Doi = {10.1103/PhysRevD.60.052003},
Key = {fds308225}
}
@article{fds356761,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of W boson angular distributions in events with
high transverse momentum jets at √s=8 TeV using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {765},
Pages = {132-153},
Year = {2017},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2016.12.005},
Abstract = {The W boson angular distribution in events with high
transverse momentum jets is measured using data collected by
the ATLAS experiment from proton–proton collisions at a
centre-of-mass energy s=8 TeV at the Large Hadron Collider,
corresponding to an integrated luminosity of 20.3 fb−1.
The focus is on the contributions to W+jets processes from
real W emission, which is achieved by studying events where
a muon is observed close to a high transverse momentum jet.
At small angular separations, these contributions are
expected to be large. Various theoretical models of this
process are compared to the data in terms of the absolute
cross-section and the angular distributions of the muon from
the leptonic W decay.},
Doi = {10.1016/j.physletb.2016.12.005},
Key = {fds356761}
}
@article{fds348982,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro,
R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
MR},
Title = {Measurement of W W / W Z → ℓ ν q q ' production with
the hadronically decaying boson reconstructed as one or two
jets in pp collisions at s = 8 TeV with ATLAS, and
constraints on anomalous gauge couplings.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {8},
Pages = {563},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5084-2},
Abstract = {This paper presents a study of the production of <i>WW</i>
or <i>WZ</i> boson pairs, with one <i>W</i> boson decaying
to e ν or μ ν and one <i>W</i> or <i>Z</i> boson decaying
hadronically. The analysis uses 20.2 fb - 1 of s = 8 TeV
<i>pp</i> collision data, collected by the ATLAS detector at
the Large Hadron Collider. Cross-sections for
<i>WW</i> / <i>WZ</i> production are measured in high- p T
fiducial regions defined close to the experimental event
selection. The cross-section is measured for the case where
the hadronically decaying boson is reconstructed as two
resolved jets, and the case where it is reconstructed as a
single jet. The transverse momentum distribution of the
hadronically decaying boson is used to search for new
physics. Observations are consistent with the Standard Model
predictions, and 95% confidence intervals are calculated for
parameters describing anomalous triple gauge-boson
couplings.},
Doi = {10.1140/epjc/s10052-017-5084-2},
Key = {fds348982}
}
@article{fds307988,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D},
Title = {Measurement of W-boson helicity fractions in top-quark
decays using cos θ*},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {674},
Number = {3},
Pages = {160-167},
Publisher = {Elsevier BV},
Year = {2009},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2009.02.040},
Abstract = {Fully reconstructed t over(t, ̄) → W+ b W- over(b, ̄)
→ ℓ ν q over(q, ̄)′ b over(b, ̄) events are used to
determine the fractions of right-handed (f+) and
longitudinally polarized (f0) W bosons produced in top-quark
decays. The helicity fractions are sensitive to the
couplings and the Dirac structure of the Wtb vertex. This
Letter reports measurements of the W-boson helicity
fractions from two different methods using data
corresponding to an integrated luminosity of 1.9 fb- 1 of p
over(p, ̄) collisions at a center-of-mass energy of 1.96
TeV collected by the CDF II detector operating at the
Fermilab Tevatron. Combining the results from the two
methods, we find f0 = 0.62 ± 0.10 (stat) ± 0.05 (syst)
under the assumption that f+ = 0, and f+ = - 0.04 ± 0.04
(stat) ± 0.03 (syst) with f0 fixed to the theoretically
expected value of 0.70. Model-independent fits are also
performed and simultaneously determine f0 = 0.66 ± 0.16
(stat) ± 0.05 (syst) and f+ = - 0.03 ± 0.06 (stat) ± 0.03
(syst). All these results are consistent with standard model
expectations. © 2009 Elsevier B.V.},
Doi = {10.1016/j.physletb.2009.02.040},
Key = {fds307988}
}
@article{fds307900,
Author = {Aaltonen, and T, and others},
Title = {Measurement of W-Boson Polarization in Top-Quark Decay in
ppbar Collisions at sqrt{s}=1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {4},
Pages = {042002},
Publisher = {American Physical Society},
Year = {2010},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.042002},
Abstract = {We report measurements of the polarization of W bosons from
top-quark decays using 2.7 fb{-1} of pp collisions collected
by the CDF II detector. Assuming a top-quark mass of
175 GeV/c{2}, three measurements are performed. A
simultaneous measurement of the fraction of longitudinal
(f{0}) and right-handed (f{+}) W bosons yields the
model-independent results f{0}=0.88±0.11(stat)±0.06(syst)
and f{+}=-0.15±0.07(stat)±0.06(syst) with a correlation
coefficient of -0.59. A measurement of f{0} [f{+}]
constraining f{+} [f{0}] to its standard model value of 0.0
[0.7] yields f{0}=0.70±0.07(stat)±0.04(syst)
[f{+}=-0.01±0.02(stat)±0.05(syst)]. All these results are
consistent with standard model expectations. We achieve the
single most precise measurements of f{0} for both the
model-independent and model-dependent determinations.},
Doi = {10.1103/PhysRevLett.105.042002},
Key = {fds307900}
}
@article{fds307627,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Measurement of W-boson polarization in top-quark decay using
the full CDF Run II data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.87.031104},
Abstract = {We measure the polarization of W bosons from top-quark (t)
decays into final states with a charged lepton and jets,
tt̄→W+bW -b̄→ℓνbqq̄′b̄, using the full Run II
data set collected by the CDF II detector, corresponding to
an integrated luminosity of 8.7 fb-1. A model-independent
method simultaneously determines the fraction of
longitudinal (f0) and right-handed (f+) W bosons to yield
f0=0.726±0. 066(stat)±0.067(syst) and f+=-0.045±0.044(stat)
±0.058(syst) with a correlation coefficient of -0.69.
Additional results are presented under various standard
model assumptions. No significant discrepancies with the
standard model are observed. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.87.031104},
Key = {fds307627}
}
@article{fds313632,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery,
M},
Title = {Measurement of Wγ and Zγ production
in pp̄ collisions at √s = 1.96 TeV},
Journal = {Physical Review Letters},
Volume = {94},
Number = {4},
Year = {2005},
Month = {February},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.94.041803},
Abstract = {The standard model predictions for Wγ and Z γ production
are tested using an integrated luminosity of 200 pb-1 of
pp̄ collision data collected at the Collider Detector at
Fermilab. The cross sections are measured by selecting
leptonic decays of the W and Z bosons, and photons with
transverse energy ET > 7 GeV that are well separated from
leptons. The production cross sections and kinematic
distributions for the Wγ and Zγ data are compared to SM
predictions. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.94.041803},
Key = {fds313632}
}
@article{fds307598,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, JF and Arik, E},
Title = {Measurement of W+W- production in pp
collisions at √s=7 TeV with the ATLAS detector and limits
on anomalous WWZ and WWγ couplings},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.87.112001},
Abstract = {This paper presents a measurement of the W+W- production
cross section in pp collisions at √s=7 TeV. The leptonic
decay channels are analyzed using data corresponding to an
integrated luminosity of 4.6 fb-1 collected with the ATLAS
detector at the Large Hadron Collider. The W+W- production
cross section σ(pp→W+W-+X) is measured to be
51.9±2.0(stat)±3.9(syst)±2.0(lumi) pb, compatible with
the Standard Model prediction of 44.7-1.9+2.1 pb. A
measurement of the normalized fiducial cross section as a
function of the leading lepton transverse momentum is also
presented. The reconstructed transverse momentum
distribution of the leading lepton is used to extract limits
on anomalous WWZ and WWγ couplings.},
Doi = {10.1103/PhysRevD.87.112001},
Key = {fds307598}
}
@article{fds322934,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and AlconadaVerzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of W+W-production in
association with one jet in proton-proton collisions at √s
= 8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {763},
Pages = {114-133},
Publisher = {Elsevier BV},
Year = {2016},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2016.10.014},
Abstract = {The production of Wboson pairs in association with one jet
in pp collisions at √s = 8 TeV is studied using data
corresponding to an integrated luminosity of 20.3
fb-1collected by the ATLAS detector during 2012 at the CERN
Large Hadron Collider. The cross section is measured in a
fiducial phase-space region defined by the presence of
exactly one electron and one muon, missing transverse
momentum and exactly one jet with a transverse momentum
above 25 GeV and a pseudorapidity of |η| <4.5. The leptons
are required to have opposite electric charge and to pass
transverse momentum and pseudorapidity requirements. The
fiducial cross section is found to be σWWfid,1-jet= 136 ±
6 (stat)± 14 (syst)± 3 (lumi) fb. In combination with a
previous measurement restricted to leptonic final states
with no associated jets, the fiducial cross section of WW
production with zero or one jet is measured to be
σWWfid,≤1-jet= 511 ±9 (stat)±26 (syst)±10 (lumi)fb.
The ratio of fiducial cross sections in final states with
one and zero jets is determined to be 0.36 ±0.05. Finally,
a total cross section extrapolated from the fiducial
measurement of WW production with zero or one associated jet
is reported. The measurements are compared to theoretical
predictions and found in good agreement.},
Doi = {10.1016/j.physletb.2016.10.014},
Key = {fds322934}
}
@article{fds356562,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA},
Title = {Measurement of W± -boson and Z-boson production
cross-sections in pp collisions at √s=2.76 TeV with the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {11},
Year = {2019},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7399-7},
Abstract = {The production cross-sections for W± and Z bosons are
measured using ATLAS data corresponding to an integrated
luminosity of 4.0 pb- 1 collected at a centre-of-mass
energy s=2.76 TeV. The decay channels W→ ℓν and Z→
ℓℓ are used, where ℓ can be an electron or a muon. The
cross-sections are presented for a fiducial region defined
by the detector acceptance and are also extrapolated to the
full phase space for the total inclusive production
cross-section. The combined (average) total inclusive
cross-sections for the electron and muon channels are:
σW+→ℓνtot=2312±26(stat.)±27(syst.)±72(lumi.)±30(extr.)pb,σW-→ℓνtot=1399±21(stat.)±17(syst.)±43(lumi.)±21(extr.)pb,σZ→ℓℓtot=323.4±9.8(stat.)±5.0(syst.)±10.0(lumi.)±5.5(extr.)pb.Measured
ratios and asymmetries constructed using these
cross-sections are also presented. These observables benefit
from full or partial cancellation of many systematic
uncertainties that are correlated between the different
measurements.},
Doi = {10.1140/epjc/s10052-019-7399-7},
Key = {fds356562}
}
@article{fds321102,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Measurement of W± and Z-boson production cross
sections in pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {759},
Pages = {601-621},
Publisher = {Elsevier BV},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2016.06.023},
Abstract = {Measurements of the W±→ℓ±ν and Z→ℓ+ℓ−
production cross sections (where ℓ±=e±,μ±) in
proton–proton collisions at s=13 TeV are presented using
data recorded by the ATLAS experiment at the Large Hadron
Collider, corresponding to a total integrated luminosity of
81 pb−1. The total inclusive W±-boson production cross
sections times the single-lepton-flavour branching ratios
are σW+tot=11.83±0.02 (stat)±0.32 (sys)±0.25 (lumi) nb
and σW−tot=8.79±0.02 (stat)±0.24 (sys)±0.18 (lumi) nb
for W+ and W−, respectively. The total inclusive Z-boson
production cross section times leptonic branching ratio,
within the invariant mass window 66<mℓℓ<116 GeV, is
σZtot=1.981±0.007 (stat)±0.038 (sys)±0.042 (lumi) nb.
The W+, W−, and Z-boson production cross sections and
cross-section ratios within a fiducial region defined by the
detector acceptance are also measured. The cross-section
ratios benefit from significant cancellation of experimental
uncertainties, resulting in σW+fid/σW−fid=1.295±0.003
(stat)±0.010 (sys) and σW±fid/σZfid=10.31±0.04
(stat)±0.20 (sys). Theoretical predictions, based on
calculations accurate to next-to-next-to-leading order for
quantum chromodynamics and to next-to-leading order for
electroweak processes and which employ different parton
distribution function sets, are compared to these
measurements.},
Doi = {10.1016/j.physletb.2016.06.023},
Key = {fds321102}
}
@article{fds356563,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira,
RA},
Title = {Measurement of W± boson production in Pb+Pb
collisions at √sNN=5.02Te with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {11},
Year = {2019},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7439-3},
Abstract = {A measurement of W± boson production in Pb+Pb collisions at
sNN=5.02Te is reported using data recorded by the ATLAS
experiment at the LHC in 2015, corresponding to a total
integrated luminosity of 0.49nb-1. The W± bosons are
reconstructed in the electron or muon leptonic decay
channels. Production yields of leptonically decaying W±
bosons, normalised by the total number of minimum-bias
events and the nuclear thickness function, are measured
within a fiducial region defined by the detector acceptance
and the main kinematic requirements. These normalised yields
are measured separately for W+ and W- bosons, and are
presented as a function of the absolute value of
pseudorapidity of the charged lepton and of the collision
centrality. The lepton charge asymmetry is also measured as
a function of the absolute value of lepton pseudorapidity.
In addition, nuclear modification factors are calculated
using the W± boson production cross-sections measured in pp
collisions. The results are compared with predictions based
on next-to-leading-order calculations with CT14 parton
distribution functions as well as with predictions obtained
with the EPPS16 and nCTEQ15 nuclear parton distribution
functions. No dependence of normalised production yields on
centrality and a good agreement with predictions are
observed for mid-central and central collisions. For
peripheral collisions, the data agree with predictions
within 1.7 (0.9) standard deviations for W- (W+)
bosons.},
Doi = {10.1140/epjc/s10052-019-7439-3},
Key = {fds356563}
}
@article{fds356594,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster,
AJ},
Title = {Measurement of W±Z production cross sections and
gauge boson polarisation in pp collisions at √s=13TeV with
the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {6},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7027-6},
Abstract = {This paper presents measurements of W±Z production cross
sections in pp collisions at a centre-of-mass energy of
13 TeV. The data were collected in 2015 and 2016 by the
ATLAS experiment at the Large Hadron Collider, and
correspond to an integrated luminosity of 36.1fb-1. The W±Z
candidate events are reconstructed using leptonic decay
modes of the gauge bosons into electrons and muons. The
measured inclusive cross section in the detector fiducial
region for a single leptonic decay mode is
σW±Z→ℓ′νℓℓfid.=63.7±1.0(stat.)±2.3(syst.)±1.4(lumi.) fb,
reproduced by the next-to-next-to-leading-order Standard
Model prediction of 61.5-1.3+1.4 fb. Cross sections for W+Z
and W-Z production and their ratio are presented as well as
differential cross sections for several kinematic
observables. An analysis of angular distributions of leptons
from decays of W and Z bosons is performed for the first
time in pair-produced events in hadronic collisions, and
integrated helicity fractions in the detector fiducial
region are measured for the W and Z bosons separately. Of
particular interest, the longitudinal helicity fraction of
pair-produced vector bosons is also measured.},
Doi = {10.1140/epjc/s10052-019-7027-6},
Key = {fds356594}
}
@article{fds307683,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
M},
Title = {Measurement of W±Z production in proton-proton
collisions At √s = 7 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {10},
Publisher = {Springer Nature},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2173-0},
Abstract = {A study of W ± Z production in proton-proton collisions at
√s = 7 TeV is presented using data corresponding to an
integrated luminosity of 4.6 fb−1 collected with the ATLAS
detector at the Large Hadron Collider in 2011. In total, 317
candidates, with a background expectation of 68 ± 10
events, are observed in double-leptonic decay final states
with electrons, muons and missing transverse momentum. The
total cross-section is determined to be be σtotWZ =
19.0+1.4−1.3 (stat.) ± 0.9(syst.) ± 0.4(lumi.) pb,
consistent with the Standard Model expectation of
17.6+1.1−1.0 pb. Limits on anomalous triple gauge boson
couplings are derived using the transverse momentum spectrum
of Z bosons in the selected events. The cross-section is
also presented as a function of Z boson transverse momentum
and diboson invariant mass.},
Doi = {10.1140/epjc/s10052-012-2173-0},
Key = {fds307683}
}
@article{fds356768,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurement of W±W± vector-boson scattering and limits on
anomalous quartic gauge couplings with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {96},
Number = {1},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.96.012007},
Abstract = {This paper presents the extended results of measurements of
W±W±jj production and limits on anomalous quartic gauge
couplings using 20.3 fb-1 of proton-proton collision data at
s=8 TeV recorded by the ATLAS detector at the Large Hadron
Collider. Events with two leptons (e or μ) with the same
electric charge and at least two jets are analyzed.
Production cross sections are determined in two fiducial
regions, with different sensitivities to the electroweak and
strong production mechanisms. An additional fiducial region,
particularly sensitive to anomalous quartic gauge coupling
parameters α4 and α5, is introduced, which allows more
stringent limits on these parameters compared to the
previous ATLAS measurement.},
Doi = {10.1103/PhysRevD.96.012007},
Key = {fds356768}
}
@article{fds307793,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D},
Title = {Measurement of Wγ and Zγ production cross sections in pp
collisions at √s=7 TeV and limits on anomalous triple
gauge couplings with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {717},
Number = {1-3},
Pages = {49-69},
Publisher = {Elsevier BV},
Year = {2012},
Month = {October},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.09.017},
Abstract = {This Letter presents measurements of l±νγ and l+l−γ
(l=e,μ) production in 1.02 fb−1 of pp collision data
recorded at s=7 TeV with the ATLAS detector at the LHC in
the first half of 2011. Events dominated by Wγ and Zγ
production with leptonic decays of the W and Z bosons are
selected, and their production cross sections and kinematic
properties are measured in several ranges of the photon
transverse energy. The results are compared to Standard
Model predictions and are used to determine limits on
anomalous WWγ and ZZγ/Zγγ couplings.},
Doi = {10.1016/j.physletb.2012.09.017},
Key = {fds307793}
}
@article{fds325780,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai,
S},
Title = {Measurement of Wγ and Zγ production in proton-proton
collisions at √s = 7 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2011},
Number = {9},
Publisher = {Springer Nature},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP09(2011)072},
Abstract = {We present studies of W and Z bosons with associated high
energy photons produced in pp collisions at √s = 7TeV. The
analysis uses 35 pb γ + X) event candidates are selected.
The kinematic distributions of the leptons and photons and
the production cross sections are measured. The data are
found to agree with Standard Model predictions that include
next-to-leading-order O(ααs) contributions. © SISSA
2011.},
Doi = {10.1007/JHEP09(2011)072},
Key = {fds325780}
}
@article{fds307635,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland,
W},
Title = {Measurement of Z boson production in Pb-Pb collisions at
sqrt[s(NN)]=2.76 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {110},
Number = {2},
Pages = {022301},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.110.022301},
Abstract = {The ATLAS experiment has observed 1995 Z boson candidates in
data corresponding to 0.15 nb(-1) of integrated
luminosity obtained in the 2011 LHC Pb+Pb run at
sqrt[s(NN)]=2.76 TeV. The Z bosons are reconstructed
via dielectron and dimuon decay channels, with a background
contamination of less than 3%. Results from the two channels
are consistent and are combined. Within the statistical and
systematic uncertainties, the per-event Z boson yield is
proportional to the number of binary collisions estimated by
the Glauber model. The elliptic anisotropy of the azimuthal
distribution of the Z boson with respect to the event plane
is found to be consistent with zero.},
Doi = {10.1103/physrevlett.110.022301},
Key = {fds307635}
}
@article{fds307712,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurement of ZZ production in leptonic final states at
sqrt[s] of 1.96 TeV at CDF.},
Journal = {Physical review letters},
Volume = {108},
Number = {10},
Pages = {101801},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.108.101801},
Abstract = {In this Letter, we present a precise measurement of the
total ZZ production cross section in pp collisions at
sqrt[s]=1.96 TeV, using data collected with the CDF II
detector corresponding to an integrated luminosity of
approximately 6 fb(-1). The result is obtained by
combining separate measurements in the four-charged
(ℓℓℓ' ℓ') and two-charged-lepton and
two-neutral-lepton (ℓℓνν) decay modes of the Z boson
pair. The combined measured cross section for pp → ZZ is
1.64(-0.38)(+0.44) pb. This is the most precise
measurement of the ZZ production cross section in 1.96 TeV
pp collisions to date.},
Doi = {10.1103/physrevlett.108.101801},
Key = {fds307712}
}
@article{fds307618,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurement of ZZ production in pp collisions at √ = 7 TeV
and limits on anomalous ZZZ and ZZγ couplings with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {3},
Publisher = {Springer Nature},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2013)128},
Abstract = {A measurement of the ZZ production cross section in
proton-proton collisions at √ = 7 TeV using data recorded
by the ATLAS experiment at the Large Hadron Collider is
presented. In a data sample corresponding to an integrated
luminosity of 4.6 fb-1 collected in 2011, events are
selected that are consistent either with two Z bosons
decaying to electrons or muons or with one Z boson decaying
to electrons or muons and a second Z boson decaying to
neutrinos. The ZZ → ℓ + ℓ - ℓ ′+ ℓ ′- and ZZ
→ ℓ + ℓ - ℓv̄v cross sections are measured in
restricted phase-space regions. These results are then used
to derive the total cross section for ZZ events produced
with both Z bosons in the mass range 66 to 116 GeV, σZZtot
= 6.7 ± 0.7 (stat.) -0.3+0.4 (stat.) ± 0.3 (lumi.) pb,
which is consistent with the Standard Model prediction of
5.89-0.18+0.22 pb calculated at next-to-leading order in
QCD. The normalized differential cross sections in bins of
various kinematic variables are presented. Finally, the
differential event yield as a function of the transverse
momentum of the leading Z boson is used to set limits on
anomalous neutral triple gauge boson couplings in ZZ
production. © 2013 Cern for the benefit of the ATLAS
collaboration.},
Doi = {10.1007/JHEP03(2013)128},
Key = {fds307618}
}
@article{fds356570,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP},
Title = {Measurement of ZZ production in the ℓℓνν final state
with the ATLAS detector in pp collisions at √s = 13
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {10},
Year = {2019},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2019)127},
Abstract = {This paper presents a measurement of ZZ production with the
ATLAS detector at the Large Hadron Collider. The measurement
is carried out in the final state with two charged leptons
and two neutrinos, using data collected during 2015 and 2016
in pp collisions at s = 13 TeV, corresponding to an
integrated luminosity of 36.1 fb−1. The integrated
cross-sections in the total and fiducial phase spaces are
measured with an uncertainty of 7% and compared with
Standard Model predictions, and differential measurements in
the fiducial phase space are reported. No significant
deviations from the Standard Model predictions are observed,
and stringent constraints are placed on anomalous couplings
corresponding to neutral triple gauge-boson interactions.
[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP10(2019)127},
Key = {fds356570}
}
@article{fds374030,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport, PP and Aloisio,
A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev,
V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Measurement of Zγγ production in pp collisions at √s=13
TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11579-8},
Abstract = {Cross-sections for the production of a Z boson in
association with two photons are measured in proton–proton
collisions at a centre-of-mass energy of 13 TeV. The data
used correspond to an integrated luminosity of 139 fb - 1
recorded by the ATLAS experiment during Run 2 of the LHC.
The measurements use the electron and muon decay channels of
the Z boson, and a fiducial phase-space region where the
photons are not radiated from the leptons. The integrated
Z(→ ℓℓ) γγ cross-section is measured with a
precision of 12% and differential cross-sections are
measured as a function of six kinematic variables of the
Zγγ system. The data are compared with predictions from MC
event generators which are accurate to up to next-to-leading
order in QCD. The cross-section measurements are used to set
limits on the coupling strengths of dimension-8 operators in
the framework of an effective field theory.},
Doi = {10.1140/epjc/s10052-023-11579-8},
Key = {fds374030}
}
@article{fds307769,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi,
E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman,
J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ},
Title = {Measurement of [Formula: see text] production with a veto on
additional central jet activity in pp collisions at
[Formula: see text] TeV using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {72},
Number = {6},
Pages = {2043},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2043-9},
Abstract = {A measurement of the jet activity in [Formula: see text]
events produced in proton-proton collisions at a
centre-of-mass energy of 7 TeV is presented, using
2.05 fb<sup>-1</sup> of integrated luminosity collected by
the ATLAS detector at the Large Hadron Collider. The
[Formula: see text] events are selected in the dilepton
decay channel with two identified <i>b</i>-jets from the top
quark decays. Events are vetoed if they contain an
additional jet with transverse momentum above a threshold in
a central rapidity interval. The fraction of events
surviving the jet veto is presented as a function of this
threshold for four different central rapidity interval
definitions. An alternate measurement is also performed, in
which events are vetoed if the scalar transverse momentum
sum of the additional jets in each rapidity interval is
above a threshold. In both measurements, the data are
corrected for detector effects and compared to the
theoretical models implemented in MC@NLO, Powheg, Alpgen and
Sherpa. The experimental uncertainties are often smaller
than the spread of theoretical predictions, allowing
deviations between data and theory to be observed in some
regions of phase space.},
Doi = {10.1140/epjc/s10052-012-2043-9},
Key = {fds307769}
}
@article{fds308073,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci,
MA},
Title = {Measurement of σ(pp̄→Z)•B(Z→ττ) in pp̄ collisions
at s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {75},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2007},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.75.092004},
Abstract = {We present a measurement of the inclusive production cross
section for Z bosons decaying to tau leptons in pp̄
collisions at s=1.96TeV. We use a channel with one
hadronically-decaying and one electronically-decaying tau.
This measurement is based on 350pb-1 of CDF Run II data.
Using a sample of 504 opposite sign eτ events with a total
expected background of 190 events, we obtain
σ(pp̄→4Z)•B(Z→ττ)=264±23(stat)
±14(syst)±15(lumi)pb, in agreement with the
next-to-next-to- leading order QCD prediction. This is the
first CDF cross section measurement using
hadronically-decaying taus in Run II. © 2007 The American
Physical Society.},
Doi = {10.1103/PhysRevD.75.092004},
Key = {fds308073}
}
@article{fds344668,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casarsa,
M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully,
JC and Cyr, D and Daronco, S and Datta, M and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher,
A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and Dituro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube,
S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Gimmell, JL and Ginsburg,
C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino,
C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez,
M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman,
J and Nagano, A and Naganoma, J and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Ranjan, N and Rappoccio, S and Reisert, B and Rekovic, V and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P},
Title = {Measurement of σχc2B(χc2→J/ψγ)/ σχc1B(χc1→J/ψγ)
in pp̄ Collisions at s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {98},
Number = {23},
Pages = {232001},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevLett.98.232001},
Abstract = {We measure the ratio of cross section times branching
fraction, Rp=σχc2B(χc2→J/ψγ)/σχc1B(χc1→J/ ψγ),
in 1.1fb-1 of pp̄ collisions at s=1.96TeV. This measurement
covers the kinematic range pT(J/ψ)>4.0GeV/c,
η(J/ψ)<1.0, and pT(γ)>1.0GeV/c. For events due to
prompt processes, we find Rp=0.395±0.016(stat)±0.015(syst).
This result represents a significant improvement in
precision over previous measurements of prompt χc1,2 hadro
production. © 2007 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.98.232001},
Key = {fds344668}
}
@article{fds347471,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Measurement of τ polarisation in Z / γ ∗ → τ τ
decays in proton-proton collisions at s = 8 TeV with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {2},
Pages = {163},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5619-1},
Abstract = {This paper presents a measurement of the polarisation of τ
leptons produced in Z / γ ∗ → τ τ decays which is
performed with a dataset of proton-proton collisions at s =
8 TeV, corresponding to an integrated luminosity of 20.2 fb
- 1 recorded with the ATLAS detector at the LHC in 2012. The
Z / γ ∗ → τ τ decays are reconstructed from a
hadronically decaying τ lepton with a single charged
particle in the final state, accompanied by a τ lepton that
decays leptonically. The τ polarisation is inferred from
the relative fraction of energy carried by charged and
neutral hadrons in the hadronic τ decays. The polarisation
is measured in a fiducial region that corresponds to the
kinematic region accessible to this analysis. The τ
polarisation extracted over the full phase space within the
Z / γ ∗ mass range of 66 < m Z / γ ∗ < 116 GeV is
found to be P τ = - 0.14 ± 0.02 ( stat ) ± 0.04 ( syst )
. It is in agreement with the Standard Model prediction of P
τ = - 0.1517 ± 0.0019 , which is obtained from the ALPGEN
event generator interfaced with the PYTHIA 6 parton shower
modelling and the TAUOLA τ decay library.},
Doi = {10.1140/epjc/s10052-018-5619-1},
Key = {fds347471}
}
@article{fds325306,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Da Barreiro Guimarães Costa and J and Bartoldus,
R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes,
GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and De Bruckman Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burghgrave,
B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey,
P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar,
CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Cherkaoui Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Measurement of χc1 and ψχc2 production with √s = 7 TeV
pp collisions at ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {7},
Pages = {1-51},
Publisher = {Springer Verlag},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2014)154},
Abstract = {The prompt and non-prompt production cross-sections for the
χc1 and χc2 charmonium states are measured in pp
collisions at √s = 7TeV with the ATLAS detector at the LHC
using 4.5 fb−1 of integrated luminosity. The χc states
are reconstructed through the radiative decay χc → J/ψγ
(with J/ψ → μ+μ−) where photons are reconstructed
from γ → e+e− conversions. The production rate of the
χc2 state relative to the χc1 state is measured for prompt
and non-prompt χc as a function of J/ψ transverse
momentum. The prompt χc cross-sections are combined with
existing measurements of prompt J/ψ production to derive
the fraction of prompt J/ψ produced in feed-down from χc
decays. The fractions of χc1 and χc2 produced in b-hadron
decays are also measured.},
Doi = {10.1007/JHEP07(2014)154},
Key = {fds325306}
}
@article{fds308172,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Measurement with the ATLAS detector of multi-particle
azimuthal correlations in p + Pb collisions at
√sNN= 5.02 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {725},
Number = {1-3},
Pages = {60-78},
Publisher = {Elsevier BV},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2013.06.057},
Abstract = {In order to study further the long-range correlations
("ridge") observed recently in p + Pb collisions at √sNN=
5.02 TeV, the second-order azimuthal anisotropy parameter of
charged particles, v2, has been measured with the cumulant
method using the ATLAS detector at the LHC. In a data sample
corresponding to an integrated luminosity of approximately 1
μb-1, the parameter v2has been obtained using two- and
four-particle cumulants over the pseudorapidity range
|η|<2.5. The results are presented as a function of
transverse momentum and the event activity, defined in terms
of the transverse energy summed over 3.1 < η <4.9 in the
direction of the Pb beam. They show features characteristic
of collective anisotropic flow, similar to that observed in
Pb + Pb collisions. A comparison is made to results obtained
using two-particle correlation methods, and to predictions
from hydrodynamic models of p +Pb collisions. Despite the
small transverse spatial extent of the p + Pb collision
system, the large magnitude of v2and its similarity to
hydrodynamic predictions provide additional evidence for the
importance of final-state effects in p + Pb reactions. ©
2013 CERN. Published by Elsevier B.V.},
Doi = {10.1016/j.physletb.2013.06.057},
Key = {fds308172}
}
@article{fds356669,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A},
Title = {Measurements of b-jet tagging efficiency with the ATLAS
detector using tt¯ events at √s=13 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {8},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2018)089},
Abstract = {The efficiency to identify jets containing b-hadrons
(b-jets) is measured using a high purity sample of
dileptonic top quark-antiquark pairs (tt¯) selected from
the 36.1 fb−1 of data collected by the ATLAS detector in
2015 and 2016 from proton-proton collisions produced by the
Large Hadron Collider at a centre-of-mass energy s=13 TeV.
Two methods are used to extract the efficiency from tt¯
events, a combinatorial likelihood approach and a
tag-and-probe method. A boosted decision tree, not using
b-tagging information, is used to select events in which two
b-jets are present, which reduces the dominant uncertainty
in the modelling of the flavour of the jets. The efficiency
is extracted for jets in a transverse momentum range from 20
to 300 GeV, with data-to-simulation scale factors calculated
by comparing the efficiency measured using collision data to
that predicted by the simulation. The two methods give
compatible results, and achieve a similar level of
precision, measuring data-to-simulation scale factors close
to unity with uncertainties ranging from 2% to 12% depending
on the jet transverse momentum.},
Doi = {10.1007/JHEP08(2018)089},
Key = {fds356669}
}
@article{fds307888,
Author = {Aaltonen, and T, and others},
Title = {Measurements of branching fraction ratios and
$CP$-asymmetries in suppressed ${B}^{-}\rightarrow
D(\rightarrow{K}^{+}{\pi}^{-}){K}^{-}$ and
${B}^{-}\rightarrow D(\rightarrow{K}^{+} \pi^{-}){\pi}^{-}$
decays},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {9},
Pages = {091504},
Publisher = {American Physical Society},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.84.091504},
Abstract = {We report the first reconstruction in hadron collisions of
the suppressed decays B-→D(→K+π-)K- and
B-→D(→K+π-)π-, sensitive to the Cabibbo-Kobayashi-Maskawa
phase γ, using data from 7 fb-1 of integrated
luminosity collected by the CDF II detector at the Tevatron
collider. We reconstruct a signal for the B-→D(→K+π-)K-
suppressed mode with a significance of 3.2 standard
deviations, and measure the ratios of the suppressed to
favored branching fractions R(K)=[22.0$\pm$8.6(stat)$\pm$2.6(syst)]×10-3,
R+(K)=[42.6$\pm$13.7(stat)$\pm$2.8(syst)]×10-3,
R-(K)=[3.8$\pm$10.3(stat)$\pm$2.7(syst)]×10-3 as well as
the direct CP-violating asymmetry A(K)=-0.82$\pm$0.44(stat)$\pm$0.09(syst)
of this mode. Corresponding quantities for
B-→D(→K+π-)π- decay are also reported.},
Doi = {10.1103/PhysRevD.84.091504},
Key = {fds307888}
}
@article{fds307926,
Author = {Aaltonen, and T, and others},
Title = {Measurements of branching fraction ratios and CP asymmetries
in $B^\pm \to D_{CP} K^\pm$ decays in hadron
collisions},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {3},
Pages = {031105},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.031105},
Abstract = {http://arxiv.org/abs/0911.0425},
Doi = {10.1103/PhysRevD.81.031105},
Key = {fds307926}
}
@article{fds356763,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurements of charge and CP asymmetries in b-hadron decays
using top-quark events collected by the ATLAS detector in pp
collisions at √s=8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {2},
Year = {2017},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2017)071},
Abstract = {Same- and opposite-sign charge asymmetries are measured in
lepton+jets tt¯ events in which a b-hadron decays
semileptonically to a soft muon, using data corresponding to
an integrated luminosity of 20.3 fb−1 from proton-proton
collisions at a centre-of-mass energy of s=√8 TeV
collected with the ATLAS detector at the Large Hadron
Collider at CERN. The charge asymmetries are based on the
charge of the lepton from the top-quark decay and the charge
of the soft muon from the semileptonic decay of a b-hadron
and are measured in a fiducial region corresponding to the
experimental acceptance. Four CP asymmetries (one mixing and
three direct) are measured and are found to be compatible
with zero and consistent with the Standard Model.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP02(2017)071},
Key = {fds356763}
}
@article{fds374213,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Dos Santos and SPA and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Measurements of differential cross sections of Higgs boson
production through gluon fusion in the H? WW*?
e?µ? final state at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {9},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11873-5},
Abstract = {Higgs boson production via gluon–gluon fusion is measured
in the WW*? e?µ? decay channel. The dataset utilized
corresponds to an integrated luminosity of 139 fb - 1
collected by the ATLAS detector from s=13 TeV
proton–proton collisions delivered by the Large Hadron
Collider between 2015 and 2018. Differential cross sections
are measured in a fiducial phase space restricted to the
production of at most one additional jet. The results are
consistent with Standard Model expectations, derived using
different Monte Carlo generators.},
Doi = {10.1140/epjc/s10052-023-11873-5},
Key = {fds374213}
}
@article{fds356657,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A},
Title = {Measurements of differential cross sections of top quark
pair production in association with jets in pp collisions at
√s=13 TeV using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {10},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2018)159},
Abstract = {Measurements of differential cross sections of top quark
pair production in association with jets by the ATLAS
experiment at the LHC are presented. The measurements are
performed as functions of the top quark transverse momentum,
the transverse momentum of the top quark-antitop quark
system and the out-of-plane transverse momentum using data
from pp collisions at s=13 TeV collected by the ATLAS
detector at the LHC in 2015 and corresponding to an
integrated luminosity of 3.2 fb−1. The top quark pair
events are selected in the lepton (electron or muon) + jets
channel. The measured cross sections, which are compared to
several predictions, allow a detailed study of top quark
production.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP10(2018)159},
Key = {fds356657}
}
@article{fds357655,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Measurements of differential cross-sections in four-lepton
events in 13 TeV proton-proton collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {7},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2021)005},
Abstract = {Measurements of four-lepton differential and integrated
fiducial cross-sections in events with two same-flavour,
opposite-charge electron or muon pairs are presented. The
data correspond to 139 fb−1 of s = 13 TeV proton-proton
collisions, collected by the ATLAS detector during Run 2 of
the Large Hadron Collider (2015–2018). The final state has
contributions from a number of interesting Standard Model
processes that dominate in different four-lepton invariant
mass regions, including single Z boson production, Higgs
boson production and on-shell ZZ production, with a complex
mix of interference terms, and possible contributions from
physics beyond the Standard Model. The differential
cross-sections include the four-lepton invariant mass
inclusively, in slices of other kinematic variables, and in
different lepton flavour categories. Also measured are
dilepton invariant masses, transverse momenta, and angular
correlation variables, in four regions of four-lepton
invariant mass, each dominated by different processes. The
measurements are corrected for detector effects and are
compared with state-of-the-art Standard Model calculations,
which are found to be consistent with the data. The Z →
4ℓ branching fraction is extracted, giving a value of
(4.41 ± 0.30) × 10−6. Constraints on effective field
theory parameters and a model based on a spontaneously
broken B − L gauge symmetry are also evaluated. Further
reinterpretations can be performed with the provided
information. [Figure not available: see fulltext.]},
Doi = {10.1007/JHEP07(2021)005},
Key = {fds357655}
}
@article{fds307847,
Author = {Aaltonen, and T, and al, E},
Title = {Measurements of Direct ${CP}$ Violating Asymmetries in
Charmless Decays of Strange Bottom Mesons and Bottom
Baryons},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {18},
Pages = {181802},
Publisher = {American Physical Society},
Year = {2011},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.181802},
Abstract = {We report measurements of direct CP-violating asymmetries in
charmless decays of neutral bottom hadrons to pairs of
charged hadrons with the upgraded Collider Detector at the
Fermilab Tevatron. Using a data sample corresponding to 1
fb(-1) of integrated luminosity, we obtain the first
measurements of direct CP violation in bottom strange
mesons, A(CP)(B(s)(0)→K(-)π(+))=+0.39±0.15(stat)±0.08(syst),
and bottom baryons, A(CP)(Λ(b)(0)→pπ(-))=+0.03±0.17(stat)±0.05(syst)
and A(CP)(Λ(b)(0)→pK(-))=+0.37±0.17(stat)±0.03(syst).
In addition, we measure CP violation in B(0)→K(+)π(-)
decays with 3.5σ significance, A(CP)(B(0)→K(+)π(-))=-0.086±0.023(stat)±0.009(syst),
in agreement with the current world average. Measurements of
branching fractions of B(s)(0)→K(+)K(-) and
B(0)→π(+)π(-) decays are also updated.},
Doi = {10.1103/PhysRevLett.106.181802},
Key = {fds307847}
}
@article{fds346169,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Measurements of direct CP-violating asymmetries in charmless
decays of bottom baryons.},
Journal = {Physical review letters},
Volume = {113},
Number = {24},
Pages = {242001},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.113.242001},
Abstract = {We report final measurements of direct CP-violating
asymmetries in charmless decays of neutral bottom hadrons to
pairs of charged hadrons with the upgraded Collider Detector
at the Fermilab Tevatron. Using the complete
√s=1.96 TeV proton-antiproton collisions data set,
corresponding to 9.3 fb⁻¹ of integrated luminosity,
we measure A(Λ(b)⁰→pπ⁻)=+0.06±0.07(stat)±0.03(syst)
and A(Λ(b)⁰→pK⁻)=-0.10±0.08(stat)±0.04(syst),
compatible with no asymmetry. In addition we measure the
CP-violating asymmetries in B(s)⁰→K⁻π⁺ and
B⁰→K⁺π⁻ decays to be A(B(s)⁰→K⁻π⁺)=+0.22±0.07(stat)±0.02(syst)
and A(B⁰→K⁺π⁻)=-0.083±0.013(stat)±0.004(syst),
respectively, which are significantly different from zero
and consistent with current world averages.},
Doi = {10.1103/physrevlett.113.242001},
Key = {fds346169}
}
@article{fds347507,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Piqueras,
DÁ and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung,
C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and da Costa, JBG and Bartoldus,
R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates,
RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer,
F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin,
PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard,
J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger,
AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr,
JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Bret, MC and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrillo-Montoya, GD and Carvalho, J and Casadei,
D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Alberich, LC and Cerqueira, AS and Cerri, A and Cerrito,
L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark,
PJ},
Title = {Measurements of electroweak [Formula: see text] production
and constraints on anomalous gauge couplings with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {7},
Pages = {474},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5007-2},
Abstract = {Measurements of the electroweak production of a <i>W</i>
boson in association with two jets at high dijet invariant
mass are performed using [Formula: see text] 7 and
8 [Formula: see text] proton-proton collision data
produced by the Large Hadron Collider, corresponding
respectively to 4.7 and 20.2 fb[Formula: see text] of
integrated luminosity collected by the ATLAS detector. The
measurements are sensitive to the production of a <i>W</i>
boson via a triple-gauge-boson vertex and include both the
fiducial and differential cross sections of the electroweak
process.},
Doi = {10.1140/epjc/s10052-017-5007-2},
Key = {fds347507}
}
@article{fds313591,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurements of fiducial and differential cross sections for
Higgs boson production in the diphoton decay channel at √s
= 8 TeV with ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Pages = {1-60},
Year = {2014},
Month = {September},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP09(2014)112},
Abstract = {Measurements of fiducial and differential cross sections are
presented for Higgs boson production in proton-proton
collisions at a centre-of-mass energy of √s = 8TeV. The
analysis is performed in the H → γγ decay channel using
20.3 fb−1 of data recorded by the ATLAS experiment at the
CERN Large Hadron Collider. The signal is extracted using a
fit to the diphoton invariant mass spectrum assuming that
the width of the resonance is much smaller than the
experimental resolution. The signal yields are corrected for
the effects of detector inefficiency and resolution. The pp
→ H → γγ fiducial cross section is measured to be 43.2
±9.4 (stat.) +3.2−2.9 (syst.) ±1.2 (lumi) fb for a Higgs
boson of mass 125.4 GeV decaying to two isolated photons
that have transverse momentum greater than 35% and 25% of
the diphoton invariant mass and each with absolute
pseudorapidity less than 2.37. Four additional fiducial
cross sections and two cross-section limits are presented in
phase space regions that test the theoretical modelling of
different Higgs boson production mechanisms, or are
sensitive to physics beyond the Standard Model. Differential
cross sections are also presented, as a function of
variables related to the diphoton kinematics and the jet
activity produced in the Higgs boson events. The observed
spectra are statistically limited but broadly in line with
the theoretical expectations.},
Doi = {10.1007/JHEP09(2014)112},
Key = {fds313591}
}
@article{fds346162,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P},
Title = {Measurements of fiducial cross-sections for [Formula: see
text] production with one or two additional b-jets in
pp collisions at [Formula: see text]=8 TeV using the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {11},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3852-4},
Abstract = {Fiducial cross-sections for [Formula: see text] production
with one or two additional <i>b</i>-jets are reported, using
an integrated luminosity of 20.3 fb[Formula: see text] of
proton-proton collisions at a centre-of-mass energy of 8
TeV at the Large Hadron Collider, collected with the ATLAS
detector. The cross-section times branching ratio for
[Formula: see text] events with at least one additional
<i>b</i>-jet is measured to be 950 [Formula: see text]
70 (stat.) [Formula: see text] (syst.) fb in the
lepton-plus-jets channel and 50 [Formula: see text]
10 (stat.) [Formula: see text] (syst.) fb in the
[Formula: see text] channel. The cross-section times
branching ratio for events with at least two additional
<i>b</i>-jets is measured to be 19.3 [Formula: see text]
3.5 (stat.) [Formula: see text] 5.7 (syst.) fb in the
dilepton channel ([Formula: see text], [Formula: see text],
and <i>ee</i>) using a method based on tight selection
criteria, and 13.5 [Formula: see text] 3.3 (stat.) [Formula:
see text] 3.6 (syst.) fb using a looser selection that
allows the background normalisation to be extracted from
data. The latter method also measures a value of 1.30
[Formula: see text] 0.33 (stat.) [Formula: see text]
0.28 (syst.)% for the ratio of [Formula: see text]
production with two additional <i>b</i>-jets to [Formula:
see text] production with any two additional jets. All
measurements are in good agreement with recent theory
predictions.},
Doi = {10.1140/epjc/s10052-015-3852-4},
Key = {fds346162}
}
@article{fds307530,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JC and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC},
Title = {Measurements of four-lepton production at the Z resonance in
pp collisions at sqrt[s] = 7 and 8 TeV with
ATLAS.},
Journal = {Physical review letters},
Volume = {112},
Number = {23},
Pages = {231806},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.112.231806},
Abstract = {Measurements of four-lepton (4ℓ, ℓ=e,μ) production
cross sections at the Z resonance in pp collisions at the
LHC with the ATLAS detector are presented. For dilepton and
four-lepton invariant mass regions m(ℓ+ℓ(-)) > 5 GeV and
80<m(4ℓ) < 100 GeV, the measured cross sections are 76 ±
18(stat) ± 4(syst) ± 1.4(lumi) fb and 107 ± 9(stat) ±
4(syst) ± 3.0(lumi) fb at sqrt[s] = 7 and 8 TeV,
respectively. By subtracting the nonresonant 4ℓ production
contributions and normalizing with Z → μ(+)μ(-) events,
the branching fraction for the Z boson decay to 4ℓ is
determined to be (3.20 ± 0.25(stat) ± 0.13(syst)) ×
10(-6), consistent with the standard model
prediction.},
Doi = {10.1103/physrevlett.112.231806},
Key = {fds307530}
}
@article{fds356782,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Measurements of four-lepton production in pp collisions at
√s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {753},
Pages = {552-572},
Year = {2016},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2015.12.048},
Abstract = {The four-lepton (4ℓ, ℓ=e,μ) production cross section is
measured in the mass range from 80 to 1000 GeV using 20.3
fb−1 of data in pp collisions at s=8 TeV collected with
the ATLAS detector at the LHC. The 4ℓ events are produced
in the decays of resonant Z and Higgs bosons and the
non-resonant ZZ continuum originating from qq¯, gg, and qg
initial states. A total of 476 signal candidate events are
observed with a background expectation of 26.2±3.6 events,
enabling the measurement of the integrated cross section and
the differential cross section as a function of the
invariant mass and transverse momentum of the four-lepton
system. In the mass range above 180 GeV, assuming the
theoretical constraint on the qq¯ production cross section
calculated with perturbative NNLO QCD and NLO electroweak
corrections, the signal strength of the gluon-fusion
component relative to its leading-order prediction is
determined to be μgg=2.4±1.0 (stat.)±0.5 (syst.)±0.8
(theory).},
Doi = {10.1016/j.physletb.2015.12.048},
Key = {fds356782}
}
@article{fds347553,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Measurements of gluon–gluon fusion and vector-boson fusion
Higgs boson production cross-sections in the
H → WW⁎ → eνμν decay channel in
pp collisions at √s=13TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {789},
Pages = {508-529},
Year = {2019},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2018.11.064},
Abstract = {Higgs boson production cross-sections in proton–proton
collisions are measured in the H→WW⁎→eνμν decay
channel. The proton–proton collision data were produced at
the Large Hadron Collider at a centre-of-mass energy of 13
TeV and recorded by the ATLAS detector in 2015 and 2016,
corresponding to an integrated luminosity of 36.1fb−1. The
product of the H→WW⁎ branching fraction times the
gluon–gluon fusion and vector-boson fusion cross-sections
are measured to be 11.4−1.1+1.2(stat.)−1.7+1.8(syst.)pb
and 0.50−0.22+0.24(stat.)±0.17(syst.)pb, respectively, in
agreement with Standard Model predictions.},
Doi = {10.1016/j.physletb.2018.11.064},
Key = {fds347553}
}
@article{fds307582,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and AbdelKhalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
M},
Title = {Measurements of Higgs boson production and couplings in
diboson final states with the ATLAS detector at the
LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {726},
Number = {1-3},
Pages = {88-119},
Publisher = {Elsevier BV},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2013.08.010},
Abstract = {Measurements are presented of production properties and
couplings of the recently discovered Higgs boson using the
decays into boson pairs, H→γγ, H→ZZ*→4ℓ and
H→WW*→ℓνℓν. The results are based on the complete
pp collision data sample recorded by the ATLAS experiment at
the CERN Large Hadron Collider at centre-of-mass energies of
s=7 TeV and s=8 TeV, corresponding to an integrated
luminosity of about 25 fb-1. Evidence for Higgs boson
production through vector-boson fusion is reported. Results
of combined fits probing Higgs boson couplings to fermions
and bosons, as well as anomalous contributions to
loop-induced production and decay modes, are presented. All
measurements are consistent with expectations for the
Standard Model Higgs boson. © 2013 CERN.},
Doi = {10.1016/j.physletb.2013.08.010},
Key = {fds307582}
}
@article{fds310326,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Measurements of Higgs boson production and couplings in the
four-lepton channel in pp collisions at center-of-mass
energies of 7 and 8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.91.012006},
Abstract = {The final ATLAS Run 1 measurements of Higgs boson production
and couplings in the decay channel H → ZZ∗ →
l+l-l'+l'-, where l, l' = e or μ, are presented. These
measurements were performed using pp collision data
corresponding to integrated luminosities of 4.5 and 20.3
fb-1 at center-of-mass energies of 7 and 8 TeV,
respectively, recorded with the ATLAS detector at the LHC.
The H → ZZ∗ → 4l signal is observed with a
significance of 8.1 standard deviations, with an expectation
of 6.2 standard deviations, at mH = 125.36 GeV, the combined
ATLAS measurement of the Higgs boson mass from the H →
γγ and H → ZZ∗ → 4l channels. The production rate
relative to the Standard Model expectation, the signal
strength, is measured in four different production
categories in the H → ZZ∗ → 4l channel. The measured
signal strength, at this mass, and with all categories
combined, is 1.44+0.40-0.33. The signal strength for Higgs
boson production in gluon fusion or in association with tt
or bb pairs is found to be 1.7+0.5-0.4, while the signal
strength for vector-boson fusion combined with WH/ZH
associated production is found to be 0.3+1.6-0.9.},
Doi = {10.1103/PhysRevD.91.012006},
Key = {fds310326}
}
@article{fds373465,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco, L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta,
D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Agaras, MN and Bogavac, D and Bosman, M},
Title = {Measurements of Higgs boson production by gluon-gluon fusion
and vector-boson fusion using H→WW*→eνμν decays in pp
collisions at Formula Presented with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032005},
Abstract = {Higgs boson production via gluon-gluon fusion and
vector-boson fusion in proton-proton collisions is measured
in the H → W W * → e ν μ ν decay channel. The Large
Hadron Collider delivered proton-proton collisions at a
center-of-mass energy of 13 TeV between 2015 and 2018, which
were recorded by the ATLAS detector, corresponding to an
integrated luminosity of 139 fb - 1 . The total cross
sections for Higgs boson production by gluon-gluon fusion
and vector-boson fusion times the H → W W * branching
ratio are measured to be 12.0 ± 1.4 and 0.75 - 0.16 + 0.19
pb , respectively, in agreement with the Standard Model
predictions of 10.4 ± 0.6 and 0.81 ± 0.02 pb . Higgs boson
production is further characterized through measurements of
Simplified Template Cross Sections in a total of 11
kinematic fiducial regions.},
Doi = {10.1103/PhysRevD.108.032005},
Key = {fds373465}
}
@article{fds356660,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Measurements of Higgs boson properties in the diphoton decay
channel with 36 fb -1 of pp collision data at
√s = 13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {5},
Year = {2018},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.98.052005},
Abstract = {Properties of the Higgs boson are measured in the two-photon
final state using 36.1 fb-1 of proton? proton collision data
recorded at ffiffi √s = 13 TeV by the ATLAS experiment at
the Large Hadron Collider. Cross-section measurements for
the production of a Higgs boson through gluon-gluon fusion,
vectorboson fusion, and in association with a vector boson
or a top-quark pair are reported. The signal strength,
defined as the ratio of the observed to the expected signal
yield, is measured for each of these production processes as
well as inclusively. The global signal strength measurement
of 0.99 ± 0.14 improves on the precision of the ATLAS
measurement at √s = 7 and 8 TeV by a factor of two.
Measurements of gluon-gluon fusion and vector-boson fusion
productions yield signal strengths compatible with the
Standard Model prediction. Measurements of simplified
template cross sections, designed to quantify the different
Higgs boson production processes in specific regions of
phase space, are reported. The cross section for the
production of the Higgs boson decaying to two isolated
photons in a fiducial region closely matching the
experimental selection of the photons is measured to be 55
± 10 fb, which is in good agreement with the Standard Model
prediction of 64 ± 2 fb. Furthermore, cross sections in
fiducial regions enriched in Higgs boson production in
vector-boson fusion or in association with large missing
transverse momentum, leptons or top-quark pairs are
reported. Differential and double-differential measurements
are performed for several variables related to the diphoton
kinematics as well as the kinematics and multiplicity of the
jets produced in association with a Higgs boson. These
differential cross sections are sensitive to higher order
QCD corrections and properties of the Higgs boson, such as
its spin and CP quantum numbers. No significant deviations
from a wide array of Standard Model predictions are
observed. Finally, the strength and tensor structure of the
Higgs boson interactions are investigated using an effective
Lagrangian, which introduces additional CP-even and CP-odd
interactions. No significant new physics contributions are
observed.},
Doi = {10.1103/PhysRevD.98.052005},
Key = {fds356660}
}
@article{fds357500,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
Title = {Measurements of Higgs bosons decaying to bottom quarks from
vector boson fusion production with the ATLAS experiment at
√s=13TeV},
Journal = {European Physical Journal C},
Volume = {81},
Number = {6},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09192-8},
Abstract = {The paper presents a measurement of the Standard Model Higgs
Boson decaying to b-quark pairs in the vector boson fusion
(VBF) production mode. A sample corresponding to 126 fb - 1
of s=13TeV proton–proton collision data, collected with
the ATLAS experiment at the Large Hadron Collider, is
analyzed utilizing an adversarial neural network for event
classification. The signal strength, defined as the ratio of
the measured signal yield to that predicted by the Standard
Model for VBF Higgs production, is measured to be
0.95-0.36+0.38 , corresponding to an observed (expected)
significance of 2.6 (2.8) standard deviations from the
background only hypothesis. The results are additionally
combined with an analysis of Higgs bosons decaying to
b-quarks, produced via VBF in association with a
photon.},
Doi = {10.1140/epjc/s10052-021-09192-8},
Key = {fds357500}
}
@article{fds352489,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Measurements of inclusive and differential cross-sections of
combined tt¯ γ and tWγ production in the eμ channel at
13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {9},
Year = {2020},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2020)049},
Abstract = {Inclusive and differential cross-sections for the production
of top quarks in association with a photon are measured with
proton-proton collision data corresponding to an integrated
luminosity of 139 fb−1. The data were collected by the
ATLAS detector at the LHC during Run 2 between 2015 and 2018
at a centre-of-mass energy of 13 TeV. The measurements are
performed in a fiducial volume defined at parton level.
Events with exactly one photon, one electron and one muon of
opposite sign, and at least two jets, of which at least one
is b-tagged, are selected. The fiducial cross-section is
measured to be 39.6−2.3+2.7 fb. Differential
cross-sections as functions of several observables are
compared with state-of-the-art Monte Carlo simulations and
next-to-leading-order theoretical calculations. These
include cross-sections as functions of photon kinematic
variables, angular variables related to the photon and the
leptons, and angular separations between the two leptons in
the event. All measurements are in agreement with the
predictions from the Standard Model. [Figure not available:
see fulltext.]},
Doi = {10.1007/JHEP09(2020)049},
Key = {fds352489}
}
@article{fds356611,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Measurements of inclusive and differential fiducial
cross-sections of tt¯ production with additional
heavy-flavour jets in proton-proton collisions at √s = 13
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {4},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2019)046},
Abstract = {This paper presents measurements of tt¯ production in
association with additional b-jets in pp collisions at the
LHC at a centre-of-mass energy of 13 TeV. The data were
recorded with the ATLAS detector and correspond to an
integrated luminosity of 36.1 fb −1 . Fiducial
cross-section measurements are performed in the dilepton and
lepton-plus-jets tt¯ decay channels. Results are presented
at particle level in the form of inclusive cross-sections of
tt¯ final states with three and four b-jets as well as
differential cross-sections as a function of global event
properties and properties of b-jet pairs. The measured
inclusive fiducial cross-sections generally exceed the tt¯
bb¯ predictions from various next-to-leading-order matrix
element calculations matched to a parton shower but are
compatible within the total uncertainties. The experimental
uncertainties are smaller than the uncertainties in the
predictions. Comparisons of state-of-the-art theoretical
predictions with the differential measurements are shown and
good agreement with data is found for most of them.[Figure
not available: see fulltext.].},
Doi = {10.1007/JHEP04(2019)046},
Key = {fds356611}
}
@article{fds356601,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos,
SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA and Pereira, RA and Arce, ATH and Ardell, RE and Arduh,
FA},
Title = {Measurements of inclusive and differential fiducial
cross-sections of tt¯ γ production in leptonic final
states at √s=13TeV in ATLAS},
Journal = {European Physical Journal C},
Volume = {79},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6849-6},
Abstract = {Inclusive and differential cross-sections for the production
of a top-quark pair in association with a photon are
measured with proton-proton collision data corresponding to
an integrated luminosity of 36.1 fb-1, collected by the
ATLAS detector at the LHC in 2015 and 2016 at a
centre-of-mass energy of 13 TeV. The measurements are
performed in single-lepton and dilepton final states in a
fiducial volume. Events with exactly one photon, one or two
leptons, a channel-dependent minimum number of jets, and at
least one b-jet are selected. Neural network algorithms are
used to separate the signal from the backgrounds. The
fiducial cross-sections are measured to be
521±9(stat.)±41(sys.)fb and 69±3(stat.)±4(sys.)fb for
the single-lepton and dilepton channels, respectively. The
differential cross-sections are measured as a function of
photon transverse momentum, photon absolute pseudorapidity,
and angular distance between the photon and its closest
lepton in both channels, as well as azimuthal opening angle
and absolute pseudorapidity difference between the two
leptons in the dilepton channel. All measurements are in
agreement with the theoretical predictions.},
Doi = {10.1140/epjc/s10052-019-6849-6},
Key = {fds356601}
}
@article{fds308069,
Author = {Abulencia, A and others},
Title = {Measurements of Inclusive W and Z Cross Sections in p anti-p
Collisions at $\sqrt{s} = 1.96$ TeV},
Journal = {J. Phys. G: Nucl. Part. Phys.},
Volume = {34},
Number = {12},
Pages = {2457-2544},
Publisher = {IOP Publishing},
Year = {2007},
url = {http://dx.doi.org/10.1088/0954-3899/34/12/001},
Abstract = {We report the first measurements of inclusive W and Z boson
cross-sections times the corresponding leptonic branching
ratios for p anti-p collisions at s**(1/2) = 1.96 TeV based
on the decays of the W and Z bosons into electrons and
muons. The data were recorded with the CDF II detector at
the Fermilab Tevatron and correspond to an integrated
luminosity of 72.0 +/- 4.3 pb-1. We test e-mu lepton
universality in W decays by measuring the ratio of the W -->
mu nu to W --> e nu cross sections and determine a value to
0.991 +/- 0.004(stat.) +/- 0.011(syst.) for the ratio of W -
l - nu couplings (g_mu/g_e). Since there is no sign of
non-universality, we combine our cross-section measurements
in the different lepton decay modes and obtain sigma_W x
Br(p anti-p --> W --> l nu) = 2.749 +/- 0.010(stat.) +/-
0.053(syst.) +/- 0.165(lum.) nb and sigma_gamma*/Z x BR(p
anti-p --> gamma*/Z --> ll) = 254.9 +/- 3.3(stat.) +/-
4.6(syst.) +/- 15.2(lum.) pb for dilepton pairs in the mass
range between 66 GeV/c2 and 116 GeV/c2. We compute the ratio
R of the W --> l nu to Z --> ll cross section taking all
correlations among channels into account and obtain R =
10.84 +/- 0.15(stat.) +/- 0.14(syst.) including a correction
for the virtual photon exchange component in our measured
gamma*/Z --> ll cross section. Based on the measured value
of R, we extract values for the W leptonic branching ratio,
Br(W --> l nu) = 0.1082 +/- 0.0022; the total width of the W
boson, Gamma(W) = 2092 +/- 42 MeV; and the ratio of W and Z
boson total widths, Gamma(W)/Gamma(Z) = 0.838 +/- 0.017. In
addition, we use our extracted value of Gamma(W) whose value
depends on various electroweak parameters and certain CKM
matrix elements to constrain the V_cs CKM matrix element,
|V_cs| = 0.976 +/- 0.030.},
Doi = {10.1088/0954-3899/34/12/001},
Key = {fds308069}
}
@article{fds356750,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Measurements of integrated and differential cross sections
for isolated photon pair production in pp collisions at √
s = 8 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {95},
Number = {11},
Year = {2017},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.95.112005},
Abstract = {A measurement of the production cross section for two
isolated photons in proton-proton collisions at a
center-of-mass energy of s=8 TeV is presented. The results
are based on an integrated luminosity of 20.2 fb-1 recorded
by the ATLAS detector at the Large Hadron Collider. The
measurement considers photons with pseudorapidities
satisfying |ηγ|<1.37 or 1.56<|ηγ|<2.37 and transverse
energies of respectively ET,1γ>40 GeV and ET,2γ>30 GeV for
the two leading photons ordered in transverse energy
produced in the interaction. The background due to hadronic
jets and electrons is subtracted using data-driven
techniques. The fiducial cross sections are corrected for
detector effects and measured differentially as a function
of six kinematic observables. The measured cross section
integrated within the fiducial volume is 16.8±0.8 pb. The
data are compared to fixed-order QCD calculations at
next-to-leading-order and next-to-next-to-leading-order
accuracy as well as next-to-leading-order computations
including resummation of initial-state gluon radiation at
next-to-next-to-leading logarithm or matched to a parton
shower, with relative uncertainties varying from 5% to
20%.},
Doi = {10.1103/PhysRevD.95.112005},
Key = {fds356750}
}
@article{fds310389,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Bessner, MF and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Measurements of jet vetoes and azimuthal decorrelations in
dijet events produced in [Formula: see text] collisions at
[Formula: see text] using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {11},
Pages = {3117},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3117-7},
Abstract = {Additional jet activity in dijet events is measured using
[Formula: see text] collisions at ATLAS at a centre-of-mass
energy of [Formula: see text], for jets reconstructed using
the [Formula: see text] algorithm with radius parameter
[Formula: see text]. This is done using variables such as
the fraction of dijet events without an additional jet in
the rapidity interval bounded by the dijet subsystem and
correlations between the azimuthal angles of the dijet s.
They are presented, both with and without a veto on
additional jet activity in the rapidity interval, as a
function of the scalar average of the transverse momenta of
the dijet s and of the rapidity interval size. The double
differential dijet cross section is also measured as a
function of the interval size and the azimuthal angle
between the dijet s. These variables probe differences in
the approach to resummation of large logarithms when
performing QCD calculations. The data are compared to
powheg, interfaced to the pythia 8 and herwig parton shower
generators, as well as to hej with and without interfacing
it to the ariadne parton shower generator. None of the
theoretical predictions agree with the data across the full
phase-space considered; however, powheg+pythia 8 and
hej+ariadne are found to provide the best agreement with the
data. These measurements use the full data sample collected
with the ATLAS detector in [Formula: see text][Formula: see
text] collisions at the LHC and correspond to integrated
luminosities of [Formula: see text] and [Formula: see text]
for data collected during 2010 and 2011,
respectively.},
Doi = {10.1140/epjc/s10052-014-3117-7},
Key = {fds310389}
}
@article{fds356742,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik,
M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurements of long-range azimuthal anisotropies and
associated Fourier coefficients for pp collisions at s =5.02
and 13 TeV and p+Pb collisions at sNN =5.02 TeV with the
ATLAS detector},
Journal = {Physical Review C},
Volume = {96},
Number = {2},
Year = {2017},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevC.96.024908},
Abstract = {ATLAS measurements of two-particle correlations are
presented for s=5.02 and 13 TeV pp collisions and for
sNN=5.02 TeV p+Pb collisions at the LHC. The correlation
functions are measured as a function of relative azimuthal
angle Δφ, and pseudorapidity separation Δη, using
charged particles detected within the pseudorapidity
interval |η|<2.5. Azimuthal modulation in the long-range
component of the correlation function, with |Δη|>2, is
studied using a template fitting procedure to remove a
"back-to-back" contribution to the correlation function that
primarily arises from hard-scattering processes. In addition
to the elliptic, cos(2Δφ), modulation observed in a
previous measurement, the pp correlation functions exhibit
significant cos(3Δφ) and cos(4Δφ) modulation. The
Fourier coefficients vn,n associated with the cos(nΔφ)
modulation of the correlation functions for n=2-4 are
measured as a function of charged-particle multiplicity and
charged-particle transverse momentum. The Fourier
coefficients are observed to be compatible with cos(nφ)
modulation of per-event single-particle azimuthal angle
distributions. The single-particle Fourier coefficients vn
are measured as a function of charged-particle multiplicity,
and charged-particle transverse momentum for n=2-4. The
integrated luminosities used in this analysis are, 64 nb-1
for the s=13 TeV pp data, 170 nb-1 for the s=5.02 TeV pp
data, and 28 nb-1 for the sNN=5.02 TeV p+Pb
data.},
Doi = {10.1103/PhysRevC.96.024908},
Key = {fds356742}
}
@article{fds313594,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurements of normalized differential cross sections for
t¯t production in pp collisions at √(s) = 7 TeV using the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {October},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.90.072004},
Abstract = {Measurements of normalized differential cross sections for
top-quark pair production are presented as a function of the
top-quark transverse momentum, and of the mass, transverse
momentum, and rapidity of the t¯t system, in proton-proton
collisions at a center-of-mass energy of √s = 7 TeV. The
data set corresponds to an integrated luminosity of 4.6
fb-1, recorded in 2011 with the ATLAS detector at the CERN
Large Hadron Collider. Events are selected in the lepton +
jets channel, requiring exactly one lepton and at least four
jets with at least one of the jets tagged as originating
from a b-quark. The measured spectra are corrected for
detector efficiency and resolution effects and are compared
to several Monte Carlo simulations and theory calculations.
The results are in fair agreement with the predictions in a
wide kinematic range. Nevertheless, data distributions are
softer than predicted for higher values of the mass of the
t¯t system and of the top-quark transverse momentum. The
measurements can also discriminate among different sets of
parton distribution functions.},
Doi = {10.1103/PhysRevD.90.072004},
Key = {fds313594}
}
@article{fds374029,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Measurements of observables sensitive to colour reconnection
in tt¯ events with the ATLAS detector at √s=
13 TeV},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11479-x},
Abstract = {A measurement of observables sensitive to effects of colour
reconnection in top-quark pair-production events is
presented using 139 fb - 1 of 13 TeV proton–proton
collision data collected by the ATLAS detector at the LHC.
Events are selected by requiring exactly one isolated
electron and one isolated muon with opposite charge and two
or three jets, where exactly two jets are required to be
b-tagged. For the selected events, measurements are
presented for the charged-particle multiplicity, the scalar
sum of the transverse momenta of the charged particles, and
the same scalar sum in bins of charged-particle
multiplicity. These observables are unfolded to the
stable-particle level, thereby correcting for migration
effects due to finite detector resolution, acceptance and
efficiency effects. The particle-level measurements are
compared with different colour reconnection models in Monte
Carlo generators. These measurements disfavour some of the
colour reconnection models and provide inputs to future
optimisation of the parameters in Monte Carlo
generators.},
Doi = {10.1140/epjc/s10052-023-11479-x},
Key = {fds374029}
}
@article{fds359028,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Pereira, RA},
Title = {Measurements of sensor radiation damage in the ATLAS inner
detector using leakage currents},
Journal = {Journal of Instrumentation},
Volume = {16},
Number = {8},
Year = {2021},
Month = {August},
url = {http://dx.doi.org/10.1088/1748-0221/16/08/P08025},
Abstract = {Non-ionizing energy loss causes bulk damage to the silicon
sensors of the ATLAS pixel and strip detectors. This damage
has important implications for data-taking operations,
charged-particle track reconstruction, detector simulations,
and physics analysis. This paper presents simulations and
measurements of the leakage current in the ATLAS pixel
detector and semiconductor tracker as a function of location
in the detector and time, using data collected in Run 1
(2010–2012) and Run 2 (2015–2018) of the Large Hadron
Collider. The extracted fluence shows a much stronger
|z|-dependence in the innermost layers than is seen in
simulation. Furthermore, the overall fluence on the second
innermost layer is significantly higher than in simulation,
with better agreement in layers at higher radii. These
measurements are important for validating the simulation
models and can be used in part to justify safety factors for
future detector designs and interventions.},
Doi = {10.1088/1748-0221/16/08/P08025},
Key = {fds359028}
}
@article{fds310339,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Measurements of spin correlation in top-antitop quark events
from proton-proton collisions at √s =7 TeV using the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.112016},
Abstract = {Measurements of spin correlation in top quark pair
production are presented using data collected with the ATLAS
detector at the LHC with proton-proton collisions at a
center-of-mass energy of 7 TeV, corresponding to an
integrated luminosity of 4.6 fb-1. Events are selected in
final states with two charged leptons and at least two jets
and in final states with one charged lepton and at least
four jets. Four different observables sensitive to different
properties of the top quark pair production mechanism are
used to extract the correlation between the top and antitop
quark spins. Some of these observables are measured for the
first time. The measurements are in good agreement with the
Standard Model prediction at next-to-leading-order
accuracy.},
Doi = {10.1103/PhysRevD.90.112016},
Key = {fds310339}
}
@article{fds307814,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
Cecco, S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier,
L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez,
T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi,
L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt,
M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
D and Weinberger, M and Wenzel, H and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T},
Title = {Measurements of the angular distributions in the decays
B→K(*)μ(+)μ(-) at CDF.},
Journal = {Physical review letters},
Volume = {108},
Number = {8},
Pages = {081807},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.108.081807},
Abstract = {We report an indirect search for nonstandard model physics
using the flavor-changing neutral current decays
B→K(*)μ(+)μ(-). We reconstruct the decays and measure
their angular distributions, as a function of
q(2)=M(μμ)(2)c(2), where M(μμ) is the dimuon mass, in
pp¯ collisions at √s=1.96 TeV using a data sample
corresponding to an integrated luminosity of 6.8 fb(-1). The
transverse polarization asymmetry A(T)(2) and the
time-reversal-odd charge-and-parity asymmetry A(im) are
measured for the first time, together with the K*
longitudinal polarization fraction F(L) and the muon
forward-backward asymmetry A(FB) for the decays
B(0)→K(*0)μ(+)μ(-) and B(+)→K(*+)μ(+)μ(-). The
B→K*μ(+)μ(-) forward-backward asymmetry in the most
sensitive kinematic regime, 1≤q(2)<6 GeV(2)/c(2), is
measured to be A(FB)=0.29(-0.23)(+0.20)(stat)±0.07(syst),
the most precise result to date. No deviations from the
standard model predictions are observed.},
Doi = {10.1103/physrevlett.108.081807},
Key = {fds307814}
}
@article{fds307710,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurements of the angular distributions of muons from Υ
decays in pp collisions at sqrt[s] = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {15},
Pages = {151802},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.108.151802},
Abstract = {The angular distributions of muons from Υ(1S,2S,3S) → μ+
μ- decays are measured using data from pp collisions at
sqrt[s] = 1.96 TeV corresponding to an integrated
luminosity of 6.7 fb(-1) and collected with the CDF II
detector at the Fermilab Tevatron. This analysis is the
first to report the full angular distributions as functions
of transverse momentum p(T) for Υ mesons in both the
Collins-Soper and s-channel helicity frames. This is also
the first measurement of the spin alignment of Υ(3S)
mesons. Within the kinematic range of Υ rapidity |y|<0.6
and p(T) up to 40 GeV/c, the angular distributions are
found to be nearly isotropic.},
Doi = {10.1103/physrevlett.108.151802},
Key = {fds307710}
}
@article{fds321109,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Measurements of the charge asymmetry in top-quark pair
production in the dilepton final state at s =8 TeV with the
ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032006},
Abstract = {Measurements of the top-antitop quark pair production charge
asymmetry in the dilepton channel, characterized by two
high-pT leptons (electrons or muons), are presented using
data corresponding to an integrated luminosity of 20.3 fb-1
from pp collisions at a center-of-mass energy s=8 TeV
collected with the ATLAS detector at the Large Hadron
Collider at CERN. Inclusive and differential measurements as
a function of the invariant mass, transverse momentum, and
longitudinal boost of the tt system are performed both in
the full phase space and in a fiducial phase space closely
matching the detector acceptance. Two observables are
studied: ACℓℓ based on the selected leptons and ACtt
based on the reconstructed tt final state. The inclusive
asymmetries are measured in the full phase space to be
ACℓℓ=0.008±0.006 and ACtt=0.021±0.016, which are in
agreement with the Standard Model predictions of
ACℓℓ=0.0064±0.0003 and ACtt=0.0111±0.0004.},
Doi = {10.1103/PhysRevD.94.032006},
Key = {fds321109}
}
@article{fds307763,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Measurements of the electron and muon inclusive
cross-sections in proton-proton collisions at √s=7TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {707},
Number = {5},
Pages = {438-458},
Publisher = {Elsevier BV},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2011.12.054},
Abstract = {This Letter presents measurements of the differential
cross-sections for inclusive electron and muon production in
proton-proton collisions at a centre-of-mass energy of
s=7TeV, using data collected by the ATLAS detector at the
LHC. The muon cross-section is measured as a function of pT
in the range 4<pT<100GeV and within pseudorapidity |η|<2.5.
In addition the electron and muon cross-sections are
measured in the range 7<pT<26GeV and within |η|<2.0,
excluding 1.37<|η|<1.52. Integrated luminosities of 1.3pb-1
and 1.4pb-1 are used for the electron and muon measurements,
respectively. After subtraction of the W/Z/γ* contribution,
the differential cross-sections are found to be in good
agreement with theoretical predictions for heavy-flavour
production obtained from Fixed Order NLO calculations with
NLL high-pT resummation, and to be sensitive to the effects
of NLL resummation. © 2011 CERN.},
Doi = {10.1016/j.physletb.2011.12.054},
Key = {fds307763}
}
@article{fds352788,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Measurements of the Higgs boson inclusive and differential
fiducial cross sections in the 4 ℓ decay channel at √s =
13 TeV},
Journal = {European Physical Journal C},
Volume = {80},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8223-0},
Abstract = {Inclusive and differential fiducial cross sections of the
Higgs boson are measured in the H→ ZZ∗→ 4 ℓ (ℓ= e,
μ) decay channel. The results are based on proton−proton
collision data produced at the Large Hadron Collider at a
centre-of-mass energy of 13 TeV and recorded by the ATLAS
detector from 2015 to 2018, equivalent to an integrated
luminosity of 139 fb - 1. The inclusive fiducial cross
section for the H→ ZZ∗→ 4 ℓ process is measured to
be σfid= 3.28 ± 0.32 fb, in agreement with the Standard
Model prediction of σfid , SM= 3.41 ± 0.18 fb.
Differential fiducial cross sections are measured for a
variety of observables which are sensitive to the production
and decay of the Higgs boson. All measurements are in
agreement with the Standard Model predictions. The results
are used to constrain anomalous Higgs boson interactions
with Standard Model particles.},
Doi = {10.1140/epjc/s10052-020-8223-0},
Key = {fds352788}
}
@article{fds321108,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Measurements of the Higgs boson production and decay rates
and constraints on its couplings from a combined ATLAS and
CMS analysis of the LHC pp collision data at √s = 7 and 8
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {8},
Publisher = {Springer Nature},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2016)045},
Abstract = {Combined ATLAS and CMS measurements of the Higgs boson
production and decay rates, as well as constraints on its
couplings to vector bosons and fermions, are presented. The
combination is based on the analysis of five production
processes, namely gluon fusion, vector boson fusion, and
associated production with a W or a Z boson or a pair of top
quarks, and of the six decay modes H → ZZ, W W, γγ,
ττ, bb, and μμ. All results are reported assuming a
value of 125.09 GeV for the Higgs boson mass, the result of
the combined measurement by the ATLAS and CMS experiments.
The analysis uses the CERN LHC proton-proton collision data
recorded by the ATLAS and CMS experiments in 2011 and 2012,
corresponding to integrated luminosities per experiment of
approximately 5 fb−1 at √s = 7 TeV and 20 fb−1 at √s
= 8 TeV. The Higgs boson production and decay rates measured
by the two experiments are combined within the context of
three generic parameterisations: two based on cross sections
and branching fractions, and one on ratios of coupling
modifiers. Several interpretations of the measurements with
more model-dependent parameterisations are also given. The
combined signal yield relative to the Standard Model
prediction is measured to be 1.09 ± 0.11. The combined
measurements lead to observed significances for the vector
boson fusion production process and for the H → ττ decay
of 5.4 and 5.5 standard deviations, respectively. The data
are consistent with the Standard Model predictions for all
parameterisations considered.},
Doi = {10.1007/JHEP08(2016)045},
Key = {fds321108}
}
@article{fds346163,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Measurements of the Higgs boson production and decay rates
and coupling strengths using pp collision data at
[Formula: see text] and 8 TeV in the ATLAS
experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {6},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3769-y},
Abstract = {Combined analyses of the Higgs boson production and decay
rates as well as its coupling strengths to vector bosons and
fermions are presented. The combinations include the results
of the analyses of the [Formula: see text] and [Formula: see
text] decay modes, and the constraints on the associated
production with a pair of top quarks and on the off-shell
coupling strengths of the Higgs boson. The results are based
on the LHC proton-proton collision datasets, with integrated
luminosities of up to 4.7 [Formula: see text] at [Formula:
see text] TeV and 20.3 [Formula: see text] at [Formula: see
text] TeV, recorded by the ATLAS detector in 2011 and 2012.
Combining all production modes and decay channels, the
measured signal yield, normalised to the Standard Model
expectation, is [Formula: see text]. The observed Higgs
boson production and decay rates are interpreted in a
leading-order coupling framework, exploring a wide range of
benchmark coupling models both with and without assumptions
on the Higgs boson width and on the Standard Model particle
content in loop processes. The data are found to be
compatible with the Standard Model expectations for a Higgs
boson at a mass of 125.36 GeV for all models
considered.},
Doi = {10.1140/epjc/s10052-015-3769-y},
Key = {fds346163}
}
@article{fds359003,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Measurements of the inclusive and differential production
cross sections of a top-quark–antiquark pair in
association with a Z boson at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {8},
Year = {2021},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09439-4},
Abstract = {Measurements of both the inclusive and differential
production cross sections of a top-quark–antiquark pair in
association with a Z boson (tt¯ Z) are presented. The
measurements are performed by targeting final states with
three or four isolated leptons (electrons or muons) and are
based on s=13 TeV proton–proton collision data with an
integrated luminosity of 139 fb - 1, recorded from 2015 to
2018 with the ATLAS detector at the CERN Large Hadron
Collider. The inclusive cross section is measured to be
σtt¯Z= 0.99 ± 0.05 (stat.) ±0.08 (syst.) pb, in
agreement with the most precise theoretical predictions. The
differential measurements are presented as a function of a
number of kinematic variables which probe the kinematics of
the tt¯ Z system. Both absolute and normalised differential
cross-section measurements are performed at particle and
parton levels for specific fiducial volumes and are compared
with theoretical predictions at different levels of
precision, based on a χ2/ ndf and p value computation.
Overall, good agreement is observed between the unfolded
data and the predictions.},
Doi = {10.1140/epjc/s10052-021-09439-4},
Key = {fds359003}
}
@article{fds310303,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Measurements of the Nuclear Modification Factor for Jets in
Pb+Pb Collisions at √(s)NN]=2.76 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {7},
Pages = {072302},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.114.072302},
Abstract = {Measurements of inclusive jet production are performed in pp
and Pb+Pb collisions at √(s)NN=2.76 TeV with the
ATLAS detector at the LHC, corresponding to integrated
luminosities of 4.0 and 0.14 nb(-1), respectively. The
jets are identified with the anti-k(t) algorithm with R=0.4,
and the spectra are measured over the kinematic range of jet
transverse momentum 32<p(T)<500 GeV and absolute
rapidity |y|<2.1 and as a function of collision centrality.
The nuclear modification factor R(AA) is evaluated, and jets
are found to be suppressed by approximately a factor of 2 in
central collisions compared to pp collisions. The R(AA)
shows a slight increase with p(T) and no significant
variation with rapidity.},
Doi = {10.1103/physrevlett.114.072302},
Key = {fds310303}
}
@article{fds347504,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke,
RN},
Title = {Measurements of the production cross section of a [Formula:
see text] boson in association with jets in pp
collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {6},
Pages = {361},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4900-z},
Abstract = {Measurements of the production cross section of a [Formula:
see text] boson in association with jets in proton-proton
collisions at [Formula: see text] TeV are presented, using
data corresponding to an integrated luminosity of
3.16 fb[Formula: see text] collected by the ATLAS
experiment at the CERN Large Hadron Collider in 2015.
Inclusive and differential cross sections are measured for
events containing a [Formula: see text] boson decaying to
electrons or muons and produced in association with up to
seven jets with [Formula: see text] GeV and [Formula: see
text]. Predictions from different Monte Carlo generators
based on leading-order and next-to-leading-order matrix
elements for up to two additional partons interfaced with
parton shower and fixed-order predictions at next-to-leading
order and next-to-next-to-leading order are compared with
the measured cross sections. Good agreement within the
uncertainties is observed for most of the modelled
quantities, in particular with the generators which use
next-to-leading-order matrix elements and the more recent
next-to-next-to-leading-order fixed-order
predictions.},
Doi = {10.1140/epjc/s10052-017-4900-z},
Key = {fds347504}
}
@article{fds351088,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Measurements of the production cross-section for a Z boson
in association with b-jets in proton-proton collisions at
√s = 13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {7},
Year = {2020},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2020)044},
Abstract = {This paper presents a measurement of the production
cross-section of a Z boson in association with b-jets, in
proton-proton collisions at s = 13 TeV with the ATLAS
experiment at the Large Hadron Collider using data
corresponding to an integrated luminosity of 35.6 fb−1.
Inclusive and differential cross-sections are measured for
events containing a Z boson decaying into electrons or muons
and produced in association with at least one or at least
two b-jets with transverse momentum pT> 20 GeV and rapidity
|y| < 2.5. Predictions from several Monte Carlo generators
based on leading-order (LO) or next-to-leading-order (NLO)
matrix elements interfaced with a parton-shower simulation
and testing different flavour schemes for the choice of
initial-state partons are compared with measured
cross-sections. The 5-flavour number scheme predictions at
NLO accuracy agree better with data than 4-flavour number
scheme ones. The 4-flavour number scheme predictions
underestimate data in events with at least one b-jet.
[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP07(2020)044},
Key = {fds351088}
}
@article{fds313576,
Author = {Aaltonen, T and González, BÃ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'Orso, M and Deluca,
C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'Errico,
M and Canto, AD and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati,
S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and Denis,
RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome,
J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel,
M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester,
WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang,
YC},
Title = {Measurements of the properties of Λc(2595),
Λc(2625), Σc(2455), and Σ
c(2520) baryons},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {84},
Number = {1},
Year = {2011},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.84.012003},
Abstract = {We report measurements of the resonance properties of Λ
c(2595)+ and Λc(2625)+ baryons in their decays to
Λc+π+π- as well as Σc(2455)++,0 and Σ c(2520)++,0
baryons in their decays to Λc+π± final states. These
measurements are performed using data corresponding to
5.2fb-1 of integrated luminosity from pp̄ collisions at
√s=1.96TeV, collected with the CDF II detector at the
Fermilab Tevatron. Exploiting the largest available charmed
baryon sample, we measure masses and decay widths with
uncertainties comparable to the world averages for Σc
states, and significantly smaller uncertainties than the
world averages for excited Λc+ states. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.84.012003},
Key = {fds313576}
}
@article{fds307674,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Measurements of the pseudorapidity dependence of the total
transverse energy in proton-proton collisions at √s = 7TeV
with ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {11},
Pages = {1-53},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP11(2012)033},
Abstract = {This paper describes measurements of the sum of the
transverse energy of particles as a function of particle
pseudorapidity, η, in proton-proton collisions at a
centre-of-mass energy, √s = 7TeV using the ATLAS detector
at the Large Hadron Collider. The measurements are performed
in the region |η| < 4.8 for two event classes: those
requiring the presence of particles with a low transverse
momentum and those requiring particles with a significant
transverse momentum. In the second dataset measurements are
made in the region transverse to the hard scatter. The
distributions are compared to the predictions of various
Monte Carlo event generators, which generally tend to
underestimate the amount of transverse energy at high |η|.
Copyright CERN.},
Doi = {10.1007/JHEP11(2012)033},
Key = {fds307674}
}
@article{fds372218,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V},
Title = {Measurements of the suppression and correlations of dijets
in Pb+Pb collisions at√sNN = 5.02
TeV},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054908},
Abstract = {Studies of the correlations of the two highest transverse
momentum (leading) jets in individual Pb+Pb collision events
can provide information about the mechanism of jet quenching
by the hot and dense matter created in such collisions. In
Pb+Pb and pp collisions at√sNN = 5.02 TeV, measurements of
the leading dijet transverse momentum (pT) correlations are
presented. Additionally, measurements in Pb+Pb collisions of
the dijet pair nuclear modification factors projected along
leading and subleading jet pT are made. The measurements are
performed using the ATLAS detector at the LHC with 260
pb−1 of pp data collected in 2017 and 2.2 nb−1 of Pb+Pb
data collected in 2015 and 2018. An unfolding procedure is
applied to the two-dimensional leading and subleading jet pT
distributions to account for experimental effects in the
measurement of both jets. Results are provided for dijets
with leading jet pT greater than 100 GeV. Measurements of
the dijet-yield-normalized xJ distributions in Pb+Pb
collisions show an increased fraction of imbalanced jets
compared to pp collisions; these measurements are in
agreement with previous measurements of the same quantity at
2.76 TeV in the overlapping kinematic range. Measurements of
the absolutely normalized dijet rate in Pb+Pb and pp
collisions are also presented, and show that balanced dijets
are significantly more suppressed than imbalanced dijets in
Pb+Pb collisions. It is observed in the measurements of the
pair nuclear modification factors that the subleading jets
are significantly suppressed relative to leading jets with
pT between 100 and 316 GeV for all centralities in Pb+Pb
collisions.},
Doi = {10.1103/PhysRevC.107.054908},
Key = {fds372218}
}
@article{fds373464,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Guillemin, T and Hryn'ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis,
DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Sanchez
Pineda, A and Sauvan, E and Selem, L and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang, R and Zhang, J and Berlendis,
S and Cheu, E and Cui, Z and Ghosh, A and Johns, KA and Lampl, W and Lindley,
RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou,
H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai,
G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost, M and Unal, M and Huseynov, N},
Title = {Measurements of the suppression and correlations of dijets
in Xe+Xe collisions at Formula Presented
TeV},
Journal = {Physical Review C},
Volume = {108},
Number = {2},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevC.108.024906},
Abstract = {Measurements of the suppression and correlations of dijets
is performed using 3 µ b − 1 of Xe+Xe data at s N N =
5.44 TeV collected with the ATLAS detector at the CERN Large
Hadron Collider. Dijets with jets reconstructed using the R
= 0.4 anti- k t algorithm are measured differentially in jet
p T over the range of 32 to 398 GeV and the centrality of
the collisions. Significant dijet momentum imbalance is
found in the most central Xe+Xe collisions, which decreases
in more peripheral collisions. Results from the measurement
of per-pair normalized and absolutely normalized dijet p T
balance are compared with previous Pb + Pb measurements at s
N N = 5.02 TeV. The differences between the dijet
suppression in Xe+Xe and Pb + Pb are further quantified by
the ratio of pair nuclear-modification factors. The results
are found to be consistent with those measured in Pb + Pb
data when compared in classes of the same event activity and
when taking into account the difference between the
center-of-mass energies of the initial parton scattering
process in Xe+Xe and Pb + Pb collisions. These results
should provide input for a better understanding of the role
of energy density, system size, path length, and
fluctuations in the parton energy loss.},
Doi = {10.1103/PhysRevC.108.024906},
Key = {fds373464}
}
@article{fds313607,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Measurements of the top quark branching ratios into channels
with leptons and quarks with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.92.072005},
Abstract = {Measurements of the branching ratios of top quark decays
into leptons and jets using events with tt (top antitop)
pairs are reported. Events were recorded with the ATLAS
detector at the LHC in pp collisions at a center-of-mass
energy of 7 TeV. The collected data sample corresponds to an
integrated luminosity of 4.6 fb-1. The measured top quark
branching ratios agree with the Standard Model predictions
within the measurement uncertainties of a few
percent.},
Doi = {10.1103/PhysRevD.92.072005},
Key = {fds313607}
}
@article{fds307668,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Measurements of the top-quark mass and the tt cross section
in the hadronic τ+jets decay channel at sqrt[s] = 1.96
TeV.},
Journal = {Physical review letters},
Volume = {109},
Number = {19},
Pages = {192001},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.109.192001},
Abstract = {We present the first direct measurement of the top-quark
mass using tt events decaying in the hadronic τ+jets decay
channel. Using data corresponding to an integrated
luminosity of 2.2 fb(-1) collected by the CDF II detector in
pp collisions at sqrt[s] = 1.96 TeV at the Fermilab
Tevatron, we measure the tt cross section, σ(tt), and the
top-quark mass, M(top). We extract M(top) from a likelihood
based on per-event probabilities calculated with
leading-order signal and background matrix elements. We
measure σ(tt) = 8.8 ± 3.3(stat) ± 2.2(syst) pb and M(top)
= 172.7 ± 9.3(stat) ± 3.7(syst) GeV/c(2).},
Doi = {10.1103/physrevlett.109.192001},
Key = {fds307668}
}
@article{fds307916,
Author = {Aaltonen, and T, and others},
Title = {Measurements of the top-quark mass using charged particle
tracking},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {3},
Pages = {032002},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.032002},
Abstract = {http://arxiv.org/abs/0910.0969},
Doi = {10.1103/PhysRevD.81.032002},
Key = {fds307916}
}
@article{fds310262,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek,
P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura,
AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro,
F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton,
AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista,
SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G},
Title = {Measurements of the Total and Differential Higgs Boson
Production Cross Sections Combining the H→γγ and
H→ZZ^{*}→4ℓ Decay Channels at sqrt[s]=8 TeV with
the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {9},
Pages = {091801},
Year = {2015},
Month = {August},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.115.091801},
Abstract = {Measurements of the total and differential cross sections of
Higgs boson production are performed using 20.3 fb^{-1}
of pp collisions produced by the Large Hadron Collider at a
center-of-mass energy of sqrt[s]=8 TeV and recorded by
the ATLAS detector. Cross sections are obtained from
measured H→γγ and H→ZZ^{*}→4ℓ event yields, which
are combined accounting for detector efficiencies, fiducial
acceptances, and branching fractions. Differential cross
sections are reported as a function of Higgs boson
transverse momentum, Higgs boson rapidity, number of jets in
the event, and transverse momentum of the leading jet. The
total production cross section is determined to be
σ_{pp→H}=33.0±5.3 (stat)±1.6 (syst) pb. The
measurements are compared to state-of-the-art
predictions.},
Doi = {10.1103/physrevlett.115.091801},
Key = {fds310262}
}
@article{fds310317,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {Measurements of the [Formula: see text] production cross
sections in association with jets with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {2},
Pages = {82},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3262-7},
Abstract = {This paper presents cross sections for the production of a
[Formula: see text] boson in association with jets, measured
in proton-proton collisions at [Formula: see text] with the
ATLAS experiment at the large hadron collider. With an
integrated luminosity of [Formula: see text], this data set
allows for an exploration of a large kinematic range,
including jet production up to a transverse momentum of
[Formula: see text] and multiplicities up to seven
associated jets. The production cross sections for [Formula:
see text] bosons are measured in both the electron and muon
decay channels. Differential cross sections for many
observables are also presented including measurements of the
jet observables such as the rapidities and the transverse
momenta as well as measurements of event observables such as
the scalar sums of the transverse momenta of the jets. The
measurements are compared to numerous QCD predictions
including next-to-leading-order perturbative calculations,
resummation calculations and Monte Carlo
generators.},
Doi = {10.1140/epjc/s10052-015-3262-7},
Key = {fds310317}
}
@article{fds307648,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Measurements of top quark pair relative differential
cross-sections with ATLAS in pp collisions at √s = 7
TeV},
Journal = {European Physical Journal C},
Volume = {73},
Number = {1},
Pages = {1-28},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2261-1},
Abstract = {Measurements are presented of differential crosss√ ections
for top quark pair production in pp collisions at s = 7 TeV
relative to the total inclusive top quark pair production
cross-section. A data sample of 2.05 fb<sup>−1</sup>
recorded by the ATLAS detector at the Large Hadron Collider
is used. Relative differential cross-sections are derived as
a function of the invariant mass, the transverse momentum
and the rapidity of the top quark pair system. Events are
selected in the lepton (electron or muon) + jets channel.
The backgroundsubtracted differential distributions are
corrected for detector effects, normalized to the total
inclusive top quark pair production cross-section and
compared to theoretical predictions. The measurement
uncertainties range typically between 10 % and 20 % and are
generally dominated by systematic effects. No significant
deviations from the Standard Model expectations are
observed.},
Doi = {10.1140/epjc/s10052-012-2261-1},
Key = {fds307648}
}
@article{fds356757,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Measurements of top quark spin observables in tt¯ events
using dilepton final states in √s=8 TeV pp collisions with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {3},
Year = {2017},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2017)113},
Abstract = {Measurements of top quark spin observables in tt¯ events
are presented based on 20.2 fb−1 of s=8 TeV proton-proton
collisions recorded with the ATLAS detector at the LHC. The
analysis is performed in the dilepton final state,
characterised by the presence of two isolated leptons
(electrons or muons). There are 15 observables, each
sensitive to a different coefficient of the spin density
matrix of tt¯ production, which are measured independently.
Ten of these observables are measured for the first time.
All of them are corrected for detector resolution and
acceptance effects back to the parton and stable-particle
levels. The measured values of the observables at parton
level are compared to Standard Model predictions at
next-to-leading order in QCD. The corrected distributions at
stable-particle level are presented and the means of the
distributions are compared to Monte Carlo predictions. No
significant deviation from the Standard Model is observed
for any observable.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP03(2017)113},
Key = {fds356757}
}
@article{fds356558,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Measurements of top-quark pair differential and
double-differential cross-sections in the ℓ +jets channel
with pp collisions at √s=13 TeV using the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {12},
Year = {2019},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7525-6},
Abstract = {Single- and double-differential cross-section measurements
are presented for the production of top-quark pairs, in the
lepton + jets channel at particle and parton level. Two
topologies, resolved and boosted, are considered and the
results are presented as a function of several kinematic
variables characterising the top and tt¯ system and jet
multiplicities. The study was performed using data from pp
collisions at centre-of-mass energy of 13 TeV collected in
2015 and 2016 by the ATLAS detector at the CERN Large Hadron
Collider (LHC), corresponding to an integrated luminosity of
36fb-1. Due to the large tt¯ cross-section at the LHC, such
measurements allow a detailed study of the properties of
top-quark production and decay, enabling precision tests of
several Monte Carlo generators and fixed-order Standard
Model predictions. Overall, there is good agreement between
the theoretical predictions and the data.},
Doi = {10.1140/epjc/s10052-019-7525-6},
Key = {fds356558}
}
@article{fds321086,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerny, K and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Measurements of top-quark pair differential cross-sections
in the lepton+jets channel in pp collisions at
[Formula: see text] using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {538},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4366-4},
Abstract = {Measurements of normalized differential cross-sections of
top-quark pair production are presented as a function of
the top-quark, [Formula: see text] system and event-level
kinematic observables in proton-proton collisions at
a centre-of-mass energy of [Formula: see text]. The
observables have been chosen to emphasize the [Formula: see
text] production process and to be sensitive to effects of
initial- and final-state radiation, to the different parton
distribution functions, and to non-resonant processes and
higher-order corrections. The dataset corresponds to an
integrated luminosity of 20.3 fb[Formula: see text],
recorded in 2012 with the ATLAS detector at the CERN Large
Hadron Collider. Events are selected in the lepton+jets
channel, requiring exactly one charged lepton and at least
four jets with at least two of the jets tagged as
originating from a <i>b</i>-quark. The measured spectra are
corrected for detector effects and are compared to several
Monte Carlo simulations. The results are in fair agreement
with the predictions over a wide kinematic range.
Nevertheless, most generators predict a harder top-quark
transverse momentum distribution at high values than what is
observed in the data. Predictions beyond NLO accuracy
improve the agreement with data at high top-quark transverse
momenta. Using the current settings and parton distribution
functions, the rapidity distributions are not well modelled
by any generator under consideration. However, the level of
agreement is improved when more recent sets of parton
distribution functions are used.},
Doi = {10.1140/epjc/s10052-016-4366-4},
Key = {fds321086}
}
@article{fds356727,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurements of top-quark pair differential cross-sections
in the lepton+jets channel in pp collisions at √s=13 TeV
using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {11},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2017)191},
Abstract = {Measurements of differential cross-sections of top-quark
pair production in fiducial phase-spaces are presented as a
function of top-quark and tt¯ system kinematic observables
in proton-proton collisions at a centre-of-mass energy of
s=13 TeV. The data set corresponds to an integrated
luminosity of 3.2 fb−1, recorded in 2015 with the ATLAS
detector at the CERN Large Hadron Collider. Events with
exactly one electron or muon and at least two jets in the
final state are used for the measurement. Two separate
selections are applied that each focus on different
top-quark momentum regions, referred to as resolved and
boosted topologies of the tt¯ final state. The measured
spectra are corrected for detector effects and are compared
to several Monte Carlo simulations by means of calculated
χ2 and p-values.},
Doi = {10.1007/JHEP11(2017)191},
Key = {fds356727}
}
@article{fds347499,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau,
CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL},
Title = {Measurements of top-quark pair differential cross-sections
in the [Formula: see text] channel in pp collisions
at [Formula: see text] TeV using the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {5},
Pages = {292},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4821-x},
Abstract = {This article presents measurements of [Formula: see text]
differential cross-sections in a fiducial phase-space
region, using an integrated luminosity of 3.2 fb[Formula:
see text] of proton-proton data at a centre-of-mass energy
of [Formula: see text] TeV recorded by the ATLAS experiment
at the LHC in 2015. Differential cross-sections are measured
as a function of the transverse momentum and absolute
rapidity of the top quark, and of the transverse momentum,
absolute rapidity and invariant mass of the [Formula: see
text] system. The [Formula: see text] events are selected by
requiring one electron and one muon of opposite electric
charge, and at least two jets, one of which must be tagged
as containing a <i>b</i>-hadron. The measured differential
cross-sections are compared to predictions of
next-to-leading order generators matched to parton showers
and the measurements are found to be consistent with all
models within the experimental uncertainties with the
exception of the Powheg-Box [Formula: see text] Herwig++
predictions, which differ significantly from the data in
both the transverse momentum of the top quark and the mass
of the [Formula: see text] system.},
Doi = {10.1140/epjc/s10052-017-4821-x},
Key = {fds347499}
}
@article{fds352201,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud,
AA and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai,
X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP},
Title = {Measurements of top-quark pair spin correlations in the eμ
channel at √s=13 TeV using pp collisions in the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {8},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8181-6},
Abstract = {A measurement of observables sensitive to spin correlations
in tt¯ production is presented, using 36.1 fb - 1 of pp
collision data at s=13 TeV recorded with the ATLAS detector
at the Large Hadron Collider. Differential cross-sections
are measured in events with exactly one electron and one
muon with opposite-sign electric charge as a function of the
azimuthal opening angle and the absolute difference in
pseudorapidity between the electron and muon candidates in
the laboratory frame. The azimuthal opening angle is also
measured as a function of the invariant mass of the tt¯
system. The measured differential cross-sections are
compared to predictions by several NLO Monte Carlo
generators and fixed-order calculations. The observed degree
of spin correlation is somewhat higher than predicted by the
generators used. The data are consistent with the prediction
of one of the fixed-order calculations at NLO, but agree
less well with higher-order predictions. Using these
leptonic observables, a search is performed for pair
production of supersymmetric top squarks decaying into
Standard Model top quarks and light neutralinos. Top squark
masses between 170 and 230 GeV are largely excluded at the
95% confidence level for kinematically allowed values of the
neutralino mass.},
Doi = {10.1140/epjc/s10052-020-8181-6},
Key = {fds352201}
}
@article{fds356764,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos,
S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez,
O},
Title = {Measurements of top-quark pair to Z-boson cross-section
ratios at √s=13 , 8, 7 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {2},
Year = {2017},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2017)117},
Abstract = {Ratios of top-quark pair to Z-boson cross sections measured
from proton-proton collisions at the LHC centre-of-mass
energies of s=13 TeV, 8 TeV, and 7 TeV are presented by the
ATLAS Collaboration. Single ratios, at a given s for the two
processes and at different s for each process, as well as
double ratios of the two processes at different s, are
evaluated. The ratios are constructed using previously
published ATLAS measurements of the tt¯ and Z-boson
production cross sections, corrected to a common phase space
where required, and a new analysis of Z → ℓ+ℓ− where
ℓ = e, μ at s=13 TeV performed with data collected in
2015 with an integrated luminosity of 3.2 fb−1.
Correlations of systematic uncertainties are taken into
account when evaluating the uncertainties in the ratios. The
correlation model is also used to evaluate the combined
cross section of the Z → e+e− and the Z → μ+μ−
channels for each s value. The results are compared to
calculations performed at next-to-next-to-leading-order
accuracy using recent sets of parton distribution functions.
The data demonstrate significant power to constrain the
gluon distribution function for the Bjorken-x values near
0.1 and the light-quark sea for x < 0.02.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP02(2017)117},
Key = {fds356764}
}
@article{fds356708,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza,
A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O},
Title = {Measurements of tt¯ differential cross-sections of highly
boosted top quarks decaying to all-hadronic final states in
pp collisions at √s =13 TeV using the ATLAS
detector},
Journal = {Physical Review D},
Volume = {98},
Number = {1},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.98.012003},
Abstract = {Measurements are made of differential cross-sections of
highly boosted pair-produced top quarks as a function of
top-quark and tt. system kinematic observables using
proton-proton collisions at a center-of-mass energy of s=13
TeV. The data set corresponds to an integrated luminosity of
36.1 fb-1, recorded in 2015 and 2016 with the ATLAS detector
at the CERN Large Hadron Collider. Events with two
large-radius jets in the final state, one with transverse
momentum pT>500 GeV and a second with pT>350 GeV, are used
for the measurement. The top-quark candidates are separated
from the multijet background using jet substructure
information and association with a b-tagged jet. The
measured spectra are corrected for detector effects to a
particle-level fiducial phase space and a parton-level
limited phase space, and are compared to several Monte Carlo
simulations by means of calculated χ2 values. The
cross-section for tt. production in the fiducial phase-space
region is 292±7(stat)±71(syst) fb, to be compared to the
theoretical prediction of 384±36 fb.},
Doi = {10.1103/PhysRevD.98.012003},
Key = {fds356708}
}
@article{fds357238,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Measurements of W + W −+ ≥ 1 jet
production cross-sections in pp collisions at √s = 13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {6},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2021)003},
Abstract = {Fiducial and differential cross-section measurements of
W+W− production in association with at least one hadronic
jet are presented. These measurements are sensitive to the
properties of electroweak-boson self-interactions and
provide a test of perturbative quantum chromodynamics and
the electroweak theory. The analysis is performed using
proton-proton collision data collected at s = 13 TeV with
the ATLAS experiment, corresponding to an integrated
luminosity of 139 fb−1. Events are selected with exactly
one oppositely charged electron-muon pair and at least one
hadronic jet with a transverse momentum of pT> 30 GeV and a
pseudorapidity of |η| < 4.5. After subtracting the
background contributions and correcting for detector
effects, the jet-inclusive W+W−+ ≥ 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections
with respect to several kinematic variables are measured.
These measurements include leptonic quantities, such as the
lepton transverse momenta and the transverse mass of the
W+W− system, as well as jet-related observables such as
the leading jet transverse momentum and the jet
multiplicity. Limits on anomalous triple-gauge-boson
couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous
amplitude is enhanced. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP06(2021)003},
Key = {fds357238}
}
@article{fds356628,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Measurements of W and Z boson production in pp collisions at
√s=5.02 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {79},
Number = {2},
Year = {2019},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6622-x},
Abstract = {Measurements of fiducial integrated and differential cross
sections for inclusive W+, W- and Z boson production are
reported. They are based on 25.0±0.5pb-1 of pp collision
data at s=5.02 TeV collected with the ATLAS detector at the
CERN Large Hadron Collider. Electron and muon decay channels
are analysed, and the combined W+, W- and Z integrated cross
sections are found to be σW+=2266±9(stat)±29(syst)±43(lumi) pb,
σW-=1401±7(stat)±18(syst)±27(lumi) pb, and
σZ=374.5±3.4(stat)±3.6(syst)±7.0(lumi) pb, in good
agreement with next-to-next-to-leading-order QCD
cross-section calculations. These measurements serve as
references for Pb+Pb interactions at the LHC at
sNN=5.02 TeV.},
Doi = {10.1140/epjc/s10052-019-6622-x},
Key = {fds356628}
}
@article{fds374027,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Measurements of W+W- production in
decay topologies inspired by searches for electroweak
supersymmetry},
Journal = {European Physical Journal C},
Volume = {83},
Number = {8},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11508-9},
Abstract = {This paper presents a measurement of fiducial and
differential cross-sections for W+W- production in
proton–proton collisions at s=13 TeV with the ATLAS
experiment at the Large Hadron Collider using a dataset
corresponding to an integrated luminosity of 139 fb - 1 .
Events with exactly one electron, one muon and no hadronic
jets are studied. The fiducial region in which the
measurements are performed is inspired by searches for the
electroweak production of supersymmetric charginos decaying
to two-lepton final states. The selected events have
moderate values of missing transverse momentum and the
‘stransverse mass’ variable mT2 , which is widely used
in searches for supersymmetry at the LHC. The ranges of
these variables are chosen so that the acceptance is
enhanced for direct W+W- production and suppressed for
production via top quarks, which is treated as a background.
The fiducial cross-section and particle-level differential
cross-sections for six variables are measured and compared
with two theoretical SM predictions from perturbative QCD
calculations.},
Doi = {10.1140/epjc/s10052-023-11508-9},
Key = {fds374027}
}
@article{fds355439,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Measurements of WH and ZH production in the H→ bb¯ decay
channel in pp collisions at 13Te with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {2},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08677-2},
Abstract = {Measurements of the Standard Model Higgs boson decaying into
a bb¯ pair and produced in association with a W or Z boson
decaying into leptons, using proton–proton collision data
collected between 2015 and 2018 by the ATLAS detector, are
presented. The measurements use collisions produced by the
Large Hadron Collider at a centre-of-mass energy of s=13Te,
corresponding to an integrated luminosity of 139fb-1. The
production of a Higgs boson in association with a W or Z
boson is established with observed (expected) significances
of 4.0 (4.1) and 5.3 (5.1) standard deviations,
respectively. Cross-sections of associated production of a
Higgs boson decaying into bottom quark pairs with an
electroweak gauge boson, W or Z, decaying into leptons are
measured as a function of the gauge boson transverse
momentum in kinematic fiducial volumes. The cross-section
measurements are all consistent with the Standard Model
expectations, and the total uncertainties vary from 30% in
the high gauge boson transverse momentum regions to 85% in
the low regions. Limits are subsequently set on the
parameters of an effective Lagrangian sensitive to
modifications of the WH and ZH processes as well as the
Higgs boson decay into bb¯.},
Doi = {10.1140/epjc/s10052-020-08677-2},
Key = {fds355439}
}
@article{fds316851,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A},
Title = {Measurements of W±Z production cross sections in pp
collisions at s =8 TeV with the ATLAS detector and limits on
anomalous gauge boson self-couplings},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {93},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {May},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.93.092004},
Abstract = {This paper presents measurements of W±Z production in pp
collisions at a center-of-mass energy of 8 TeV. The gauge
bosons are reconstructed using their leptonic decay modes
into electrons and muons. The data were collected in 2012 by
the ATLAS experiment at the Large Hadron Collider and
correspond to an integrated luminosity of 20.3 fb-1. The
measured inclusive cross section in the detector fiducial
region is σW±Z→ ′ν=35.1±0.9(stat)±0.8(sys)±0.8(lumi)
fb, for one leptonic decay channel. In comparison, the
next-to-leading-order Standard Model expectation is
30.0±2.1 fb. Cross sections for W+Z and W-Z production and
their ratio are presented as well as differential cross
sections for several kinematic observables. Limits on
anomalous triple gauge boson couplings are derived from the
transverse mass spectrum of the W±Z system. From the
analysis of events with a W and a Z boson associated with
two or more forward jets an upper limit at 95% confidence
level on the W±Z scattering cross section of 0.63 fb, for
each leptonic decay channel, is established, while the
Standard Model prediction at next-to-leading order is
0.13±0.01 fb. Limits on anomalous quartic gauge boson
couplings are also extracted.},
Doi = {10.1103/PhysRevD.93.092004},
Key = {fds316851}
}
@article{fds307597,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Measurements of Wγ and Zγ production in pp collisions at
√s=7 TeV with the ATLAS detector at the
LHC},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.87.112003},
Abstract = {The integrated and differential fiducial cross sections for
the production of a W or Z boson in association with a
high-energy photon are measured using pp collisions at
√s=7 TeV. The analyses use a data sample with an
integrated luminosity of 4.6 fb-1 collected by the ATLAS
detector during the 2011 LHC data-taking period. Events are
selected using leptonic decays of the W and Z bosons
[W(eν,μν) and Z(e+e-, μ+μ-,νν¯)] with the
requirement of an associated isolated photon. The data are
used to test the electroweak sector of the Standard Model
and search for evidence for new phenomena. The measurements
are used to probe the anomalous WWγ, ZZγ, and Zγγ
triple-gauge-boson couplings and to search for the
production of vector resonances decaying to Zγ and Wγ. No
deviations from Standard Model predictions are observed and
limits are placed on anomalous triple-gauge-boson couplings
and on the production of new vector meson
resonances.},
Doi = {10.1103/PhysRevD.87.112003},
Key = {fds307597}
}
@article{fds317304,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Measurements of Zγ and Zγγ production in pp collisions at
s =8 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
ISSN = {2470-0010},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112002},
Abstract = {The production of Z bosons with one or two isolated
high-energy photons is studied using pp collisions at s=8
TeV. The analyses use a data sample with an integrated
luminosity of 20.3 fb-1 collected by the ATLAS detector
during the 2012 LHC data taking. The Zγ and Zγγ
production cross sections are measured with leptonic (e+e-,
μ+μ-, νν) decays of the Z boson, in extended fiducial
regions defined in terms of the lepton and photon
acceptance. They are then compared to cross-section
predictions from the Standard Model, where the sources of
the photons are radiation off initial-state quarks and
radiative Z-boson decay to charged leptons, and from
fragmentation of final-state quarks and gluons into photons.
The yields of events with photon transverse energy ET>250
GeV from +-γ events and with ET>400 GeV from ννγ events
are used to search for anomalous triple gauge-boson
couplings ZZγ and Zγγ. The yields of events with diphoton
invariant mass mγγ>200 GeV from +-γγ events and with
mγγ>300 GeV from ννγγ events are used to search for
anomalous quartic gauge-boson couplings ZZγγ and Zγγγ.
No deviations from Standard Model predictions are observed
and limits are placed on parameters used to describe
anomalous triple and quartic gauge-boson
couplings.},
Doi = {10.1103/PhysRevD.93.112002},
Key = {fds317304}
}
@article{fds356767,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Measurements of ψ(2S) and X(3872) → J/ψπ +
π − production in pp collisions at √s=8 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {1},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2017)117},
Abstract = {Differential cross sections are presented for the prompt and
non-prompt production of the hidden-charm states X(3872) and
ψ(2S), in the decay mode J/ψπ+π−, measured using 11.4
fb−1 of pp collisions at s=8 TeV by the ATLAS detector at
the LHC. The ratio of cross-sections X(3872)/ψ(2S) is also
given, separately for prompt and non-prompt components, as
well as the non-prompt fractions of X(3872) and ψ(2S).
Assuming independent single effective lifetimes for
non-prompt X(3872) and ψ(2S) production gives
RB=ℬ(B→X(3872)+any)ℬ(X(3872)→J/ψπ+π−)/ℬ(B→ψ(2S)+any)ℬ(ψ(2S)→J/ψπ+π−)=(3.95±0.32(stat)±0.08(sys))×10−2
separating short- and long-lived contributions, assuming
that the short-lived component is due to Bc decays, gives RB
= (3.57 ± 0.33(stat) ± 0.11(sys)) × 10−2, with the
fraction of non-prompt X(3872) produced via Bc decays for
pT(X(3872)) > 10 GeV being (25 ± 13(stat) ± 2(sys) ±
5(spin))%. The distributions of the dipion invariant mass in
the X(3872) and ψ(2S) decays are also measured and compared
to theoretical predictions.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP01(2017)117},
Key = {fds356767}
}
@article{fds347536,
Author = {Shega, JW and Sunkara, PD and Kotwal, A and Kern, DW and Henning, SL and McClintock, MK and Schumm, P and Waite, LJ and Dale,
W},
Title = {Measuring cognition: the Chicago Cognitive Function Measure
in the National Social Life, Health and Aging Project, Wave
2.},
Journal = {The journals of gerontology. Series B, Psychological
sciences and social sciences},
Volume = {69 Suppl 2},
Pages = {S166-S176},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1093/geronb/gbu106},
Abstract = {<h4>Objectives</h4>To describe the development of a
multidimensional test of cognition for the National Social
life, Health and Aging Project (NSHAP), the Chicago
Cognitive Function Measure (CCFM).<h4>Method</h4>CCFM
development included 3 steps: (a) A pilot test of the
Montreal Cognitive Assessment (MoCA) to create a standard
protocol, choose specific items, reorder items, and improve
clarity; (b) integration into a CAPI-based format; and (c)
evaluation of the performance of the CCFM in the field. The
CCFM was subsequently incorporated into NSHAP, Wave 2 (n =
3,377).<h4>Results</h4>The pre-test (n = 120) mean age was
71.35 (SD 8.40); 53% were female, 69% white, and 70% with
college or greater education. The MoCA took an average of
15.6min; the time for the CCFM was 12.0 min. CCFM scores
(0-20) can be used as a continuous outcome or to adjust for
cognition in a multivariable analysis. CCFM scores were
highly correlated with MoCA scores (r = .973). Modeling
projects MoCA scores from CCFM scores using the equation:
MoCA = (1.14 × CCFM) + 6.83. In Wave 2, the overall
weighted mean CCFM score was 13.9 (SE 0.13).<h4>Discussion</h4>A
survey-based adaptation of the MoCA was successfully
integrated into a nationally representative sample of older
adults, NSHAP Wave 2.},
Doi = {10.1093/geronb/gbu106},
Key = {fds347536}
}
@article{fds355713,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling,
J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
S and Balasubramanian, R and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton,
AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso,
MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
Bylund, O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhatta, S and Bhattacharya, DS and Bhattarai,
P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann,
D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman, M and Bisanz, T and Biswal, JP and Biswas,
D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bogavac, D and Bogdanchikov,
AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler,
S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton,
CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati,
L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carratta,
G and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny,
K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chatterjee, M and Chau, CC and Che, S and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen,
Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias,
TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC},
Title = {Medium-Induced Modification of Z-Tagged Charged Particle
Yields in Pb+Pb Collisions at 5.02 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {126},
Number = {7},
Pages = {072301},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.126.072301},
Abstract = {The yield of charged particles opposite to a Z boson with
large transverse momentum (p_{T}) is measured in
260 pb^{-1} of pp and 1.7 nb^{-1} of Pb+Pb
collision data at 5.02 TeV per nucleon pair recorded with
the ATLAS detector at the Large Hadron Collider. The Z boson
tag is used to select hard-scattered partons with specific
kinematics, and to observe how their showers are modified as
they propagate through the quark-gluon plasma created in
Pb+Pb collisions. Compared with pp collisions,
charged-particle yields in Pb+Pb collisions show significant
modifications as a function of charged-particle p_{T} in a
way that depends on event centrality and Z boson p_{T}. The
data are compared with a variety of theoretical calculations
and provide new information about the medium-induced energy
loss of partons in a p_{T} regime difficult to measure
through other channels.},
Doi = {10.1103/physrevlett.126.072301},
Key = {fds355713}
}
@article{fds362043,
Author = {Bauer, M and Neubert, M},
Title = {Minimal Leptoquark Explanation for the R_{D^{(*)}}, R_{K},
and (g-2)_{μ} Anomalies.},
Journal = {Physical review letters},
Volume = {116},
Number = {14},
Pages = {141802},
Publisher = {Springer Science and Business Media LLC},
Year = {2016},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.116.141802},
Abstract = {We show that by adding a single new scalar particle to the
standard model, a TeV-scale leptoquark with the quantum
numbers of a right-handed down quark, one can explain in a
natural way three of the most striking anomalies of particle
physics: the violation of lepton universality in B[over
¯]→K[over ¯]ℓ^{+}ℓ^{-} decays, the enhanced B[over
¯]→D^{(*)}τν[over ¯] decay rates, and the anomalous
magnetic moment of the muon. Constraints from other
precision measurements in the flavor sector can be satisfied
without fine-tuning. Our model predicts enhanced B[over
¯]→K[over ¯]^{(*)}νν[over ¯] decay rates and a
new-physics contribution to B_{s}-B[over ¯]_{s} mixing
close to the current central fit value.},
Doi = {10.1103/physrevlett.116.141802},
Key = {fds362043}
}
@article{fds347552,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Arduh, FA},
Title = {Modelling radiation damage to pixel sensors in the ATLAS
detector},
Journal = {Journal of Instrumentation},
Volume = {14},
Number = {6},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1088/1748-0221/14/06/P06012},
Abstract = {Silicon pixel detectors are at the core of the current and
planned upgrade of the ATLAS experiment at the LHC. Given
their close proximity to the interaction point, these
detectors will be exposed to an unprecedented amount of
radiation over their lifetime. The current pixel detector
will receive damage from non-ionizing radiation in excess of
1015 1 MeV neq/cm2, while the pixel detector designed for
the high-luminosity LHC must cope with an order of magnitude
larger fluence. This paper presents a digitization model
incorporating effects of radiation damage to the pixel
sensors. The model is described in detail and predictions
for the charge collection efficiency and Lorentz angle are
compared with collision data collected between 2015 and 2017
(≤ 10 1 MeV neq/cm2).},
Doi = {10.1088/1748-0221/14/06/P06012},
Key = {fds347552}
}
@article{fds346220,
Author = {Kothekar, V and Kotwal, A},
Title = {Molecular mechanics simulation of the interaction of
estrogen receptor with estrogen regulatory
element.},
Journal = {Indian journal of biochemistry & biophysics},
Volume = {29},
Number = {4},
Pages = {322-329},
Year = {1992},
Month = {August},
Abstract = {A model for the interaction of 31 amino acid fragment
(protein) from DNA binding domain of human estrogen receptor
(hER) with a five base pair DNA sequence 5'GGTCA 3' from
estrogen regulatory element (ERE) has been obtained using a
step-wise procedure based on structural data on model
peptides, DNA binding domain of hER, steric constrains
imposed by tetrahedral coordination of the Cys sulphurs with
zinc ion and classical secondary structural elements.
Structure of the protein as well as its complex with DNA is
obtained by energy minimization followed by refinement by
molecular mechanics. The complex is stabilized by H-bonds
between Lys22, Lys26 and Arg27 with DNA bases G2, T3 and T6.
Lys22 also made H-bond with the backbone of G2. The backbone
of Cys18 H-bonded with N7 of G1. DNA was in distorted B form
and showed evidence of protein-induced conformational
changes.},
Key = {fds346220}
}
@article{fds310372,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Monitoring and data quality assessment of the ATLAS liquid
argon calorimeter},
Journal = {Journal of Instrumentation},
Volume = {9},
Number = {7},
Pages = {P07024-P07024},
Publisher = {IOP Publishing},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1088/1748-0221/9/07/P07024},
Abstract = {The liquid argon calorimeter is a key component of the ATLAS
detector installed at the CERN Large Hadron Collider. The
primary purpose of this calorimeter is the measurement of
electron and photon kinematic properties. It also provides a
crucial input for measuring jets and missing transverse
momentum. An advanced data monitoring procedure was designed
to quickly identify issues that would affect detector
performance and ensure that only the best quality data are
used for physics analysis. This article presents the
validation procedure developed during the 2011 and 2012 LHC
data-taking periods, in which more than 98% of the
proton-proton luminosity recorded by ATLAS at a
centre-of-mass energy of 7-8 TeV had calorimeter data
quality suitable for physics analysis. © CERN 2014 for the
benefit of the ATLAS collaboration.},
Doi = {10.1088/1748-0221/9/07/P07024},
Key = {fds310372}
}
@article{fds347539,
Author = {Nair, V and Sharma, A and Kotwal, J and Bhikshapathy, M and Mishra, DK and Das, S and Sharma, S and Kapoor, R and Singh, J and Nair, V and Uday, Y and Kotwal, A},
Title = {Monitoring of response to therapy with imatinib mesylate in
Chronic Myeloid Leukemia in chronic phase
(CML-CP).},
Journal = {Medical journal, Armed Forces India},
Volume = {70},
Number = {4},
Pages = {315-320},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1016/j.mjafi.2014.07.005},
Abstract = {<h4>Background</h4>The BCR-ABL tyrosine kinase is a well
validated therapeutic target in Chronic Myeloid Leukemia
(CML). Imatinib mesylate (IM), a tyrosine kinase inhibitor
is highly effective in the treatment of chronic phase CML.
BCR - ABL transcripts have been well established as a
molecular marker to document response to therapy in CML.
Periodic monitoring of this marker helps in evolving
therapeutic strategies with IM and also in diagnosing early
relapse. This study was undertaken to monitor therapeutic
response to IM in CML in chronic phase (CML-CP) by assessing
BCR-ABL by real time quantitative PCR (RQ-PCR) techniques
and to determine the effectiveness of the Indian generic
IM.<h4>Methods</h4>One hundred consecutive patients of CML
in chronic phase (CML-CP) were treated with an Indian
generic of IM. Eighty-five patients were evaluable at 12
months of therapy. At entry, diagnosis of CML-CP was
confirmed by FISH and RQ-PCR. Response to therapy was
monitored by assessing BCR-ABL levels by RQ-PCR at 6 and 12
months of therapy. Regular follow up of patients was done to
evaluate the safety profile of IM used in these
patients.<h4>Results</h4>Complete hematological response
(CHR) rates at 3, 6, 9 and 12 months were 92%, 94%, 100% and
100% respectively. The total molecular response at 12 months
was 43.52% of which complete molecular response (CMR) was
noted in 17.64% and major molecular response (MMR) was
observed in 25.88%. A cumulative survival probability of 0.8
was observed.<h4>Conclusion</h4>The Indian generic molecule
of IM is effective in the treatment of CML-CP. The cost of
Indian generic molecule is less than Rs. 10,000 per month
there by making this affordable for large number of CML-CP
patients in India.},
Doi = {10.1016/j.mjafi.2014.07.005},
Key = {fds347539}
}
@article{fds307619,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
OK and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer,
F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Multi-channel search for squarks and gluinos in [Formula:
see text]pp collisions with the ATLAS detector at the
LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {3},
Pages = {2362},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2362-5},
Abstract = {A search for supersymmetric particles in final states with
zero, one, and two leptons, with and without jets identified
as originating from <i>b</i>-quarks, in 4.7 fb<sup>-1</sup>
of [Formula: see text]<i>pp</i> collisions produced by the
Large Hadron Collider and recorded by the ATLAS detector is
presented. The search uses a set of variables carrying
information on the event kinematics transverse and parallel
to the beam line that are sensitive to several topologies
expected in supersymmetry. Mutually exclusive final states
are defined, allowing a combination of all channels to
increase the search sensitivity. No deviation from the
Standard Model expectation is observed. Upper limits at
95 % confidence level on visible cross-sections for the
production of new particles are extracted. Results are
interpreted in the context of the constrained minimal
supersymmetric extension to the Standard Model and in
supersymmetry-inspired models with diverse,
high-multiplicity final states.},
Doi = {10.1140/epjc/s10052-013-2362-5},
Key = {fds307619}
}
@article{fds358347,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Muon reconstruction and identification efficiency in ATLAS
using the full Run 2 pp collision data set at √s=13
TeV},
Journal = {European Physical Journal C},
Volume = {81},
Number = {7},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09233-2},
Abstract = {This article documents the muon reconstruction and
identification efficiency obtained by the ATLAS experiment
for 139 fb - 1 of pp collision data at s=13 TeV collected
between 2015 and 2018 during Run 2 of the LHC. The increased
instantaneous luminosity delivered by the LHC over this
period required a reoptimisation of the criteria for the
identification of prompt muons. Improved and newly developed
algorithms were deployed to preserve high muon
identification efficiency with a low misidentification rate
and good momentum resolution. The availability of large
samples of Z→ μμ and J/ ψ→ μμ decays, and the
minimisation of systematic uncertainties, allows the
efficiencies of criteria for muon identification, primary
vertex association, and isolation to be measured with an
accuracy at the per-mille level in the bulk of the phase
space, and up to the percent level in complex kinematic
configurations. Excellent performance is achieved over a
range of transverse momenta from 3 GeV to several hundred
GeV, and across the full muon detector acceptance of | η| <
2.7.},
Doi = {10.1140/epjc/s10052-021-09233-2},
Key = {fds358347}
}
@article{fds310384,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson,
M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio,
G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker,
OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella,
G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat,
P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley,
AG and Buda, SI and Budagov, IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiarella,
V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke,
RN},
Title = {Muon reconstruction efficiency and momentum resolution of
the ATLAS experiment in proton-proton collisions at
[Formula: see text] TeV in 2010.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {9},
Pages = {3034},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3034-9},
Abstract = {This paper presents a study of the performance of the muon
reconstruction in the analysis of proton-proton collisions
at [Formula: see text] TeV at the LHC, recorded by the
ATLAS detector in 2010. This performance is described in
terms of reconstruction and isolation efficiencies and
momentum resolutions for different classes of reconstructed
muons. The results are obtained from an analysis of
[Formula: see text] meson and [Formula: see text] boson
decays to dimuons, reconstructed from a data sample
corresponding to an integrated luminosity of 40 pb[Formula:
see text]. The measured performance is compared to Monte
Carlo predictions and deviations from the predicted
performance are discussed.},
Doi = {10.1140/epjc/s10052-014-3034-9},
Key = {fds310384}
}
@article{fds316854,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Muon reconstruction performance of the ATLAS detector in
proton-proton collision data at [Formula: see
text]=13 TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {292},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4120-y},
Abstract = {This article documents the performance of the ATLAS muon
identification and reconstruction using the LHC dataset
recorded at [Formula: see text] TeV in 2015. Using a large
sample of [Formula: see text] and [Formula: see text] decays
from 3.2 fb[Formula: see text] of <i>pp</i> collision data,
measurements of the reconstruction efficiency, as well as of
the momentum scale and resolution, are presented and
compared to Monte Carlo simulations. The reconstruction
efficiency is measured to be close to [Formula: see text]
over most of the covered phase space ([Formula: see text]
and [Formula: see text] GeV). The isolation efficiency
varies between 93 and [Formula: see text] depending on the
selection applied and on the momentum of the muon. Both
efficiencies are well reproduced in simulation. In the
central region of the detector, the momentum resolution is
measured to be [Formula: see text] ([Formula: see text]) for
muons from [Formula: see text] ([Formula: see text]) decays,
and the momentum scale is known with an uncertainty of
[Formula: see text]. In the region [Formula: see text], the
[Formula: see text] resolution for muons from [Formula: see
text] decays is [Formula: see text] while the precision of
the momentum scale for low-[Formula: see text] muons from
[Formula: see text] decays is about [Formula: see
text].},
Doi = {10.1140/epjc/s10052-016-4120-y},
Key = {fds316854}
}
@article{fds374214,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez,
MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen,
T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez,
O and Arnold, H and Tame, ZPA and Artoni, G and Asada, H and Asai, K and Asai,
S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi,
S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Bunka, AT and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr,
JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán,
SC and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea,
G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti,
M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo,
MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron,
S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter,
JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Moursli, RCE and Cheu, E and Cheung, K and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A},
Title = {New techniques for jet calibration with the ATLAS
detector},
Journal = {The European Physical Journal C},
Volume = {83},
Number = {8},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11837-9},
Abstract = {<jats:title>Abstract</jats:title><jats:p>A determination of
the jet energy scale is presented using proton–proton
collision data with a centre-of-mass energy of
<jats:inline-formula><jats:alternatives><jats:tex-math>$$\sqrt{s}=13$$</jats:tex-math>??
<mml:mrow> <mml:msqrt> <mml:mi>s</mml:mi> </mml:msqrt>
<mml:mo>=</mml:mo> <mml:mn>13</mml:mn> </mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula> TeV,
corresponding to an integrated luminosity of 140
fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
<mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
<mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
</mml:math></jats:alternatives></jats:inline-formula>
collected using the ATLAS detector at the LHC. Jets are
reconstructed using the ATLAS particle-flow method that
combines charged-particle tracks and topo-clusters formed
from energy deposits in the calorimeter cells. The
anti-<jats:inline-formula><jats:alternatives><jats:tex-math>$$k_\textrm{t}$$</jats:tex-math>??
<mml:msub> <mml:mi>k</mml:mi> <mml:mtext>t</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
jet algorithm with radius parameter <jats:inline-formula><jats:alternatives><jats:tex-math>$$R=0.4$$</jats:tex-math>??
<mml:mrow> <mml:mi>R</mml:mi> <mml:mo>=</mml:mo>
<mml:mn>0.4</mml:mn> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula>
is used to define the jet. Novel jet energy scale
calibration strategies developed for the LHC Run 2 are
reported that lay the foundation for the jet calibration in
Run 3. Jets are calibrated with a series of simulation-based
corrections, including state-of-the-art techniques in jet
calibration such as machine learning methods and novel in
situ calibrations to achieve better performance than the
baseline calibration derived using up to 81
fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
<mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
<mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
</mml:math></jats:alternatives></jats:inline-formula> of Run
2 data. The performance of these new techniques is then
examined in the in situ measurements by exploiting the
transverse momentum balance between a jet and a reference
object. The <jats:italic>b</jats:italic>-quark jet energy
scale using particle flow jets is measured for the first
time with around 1% precision using <jats:inline-formula><jats:alternatives><jats:tex-math>$$\gamma
$$</jats:tex-math>?? <mml:mi>γ</mml:mi>
</mml:math></jats:alternatives></jats:inline-formula>+jet
events.</jats:p>},
Doi = {10.1140/epjc/s10052-023-11837-9},
Key = {fds374214}
}
@article{fds310116,
Author = {Hays, C and Kotwal, A and Stelzer-Chilton, O},
Title = {New techniques in the search for Z' bosons and other neutral
resonances},
Journal = {Modern Physics Letters A},
Volume = {24},
Number = {30},
Pages = {2387-2403},
Year = {2009},
Month = {September},
url = {http://dx.doi.org/10.1142/S021773230903179X},
Abstract = {The search for neutral resonances at the energy frontier has
a long and illustrious history, resulting in multiple
discoveries. The canonical search scans the reconstructed
invariant mass distribution of identified fermion pairs. Two
recent analyses from the CDF experiment at the Fermilab
Tevatron have applied novel methods to resonance searches.
One analysis uses simulated templates to fit the inverse
mass distribution of muon pairs, a quantity with
approximately constant resolution for momenta measured with
a tracking detector. The other analysis measures the angular
distribution of electron pairs as a function of dielectron
mass, gaining sensitivity over a probe of the mass spectrum
alone. After reviewing several models that predict new
neutral resonances, we discuss these CDF analyses and
potential future applications. © 2009 World Scientific
Publishing Company.},
Doi = {10.1142/S021773230903179X},
Key = {fds310116}
}
@article{fds347530,
Author = {Kotwal, A and Biswas, D and Kakati, B and Bahadur, H and Gupta,
N},
Title = {Non traumatic keratitis due to colletotrichum coccodes: a
case report.},
Journal = {Journal of clinical and diagnostic research :
JCDR},
Volume = {9},
Number = {2},
Pages = {DD01-DD02},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.7860/jcdr/2015/10843.5529},
Abstract = {Colletotrichum species, a rare and emerging fungus is a
well- known plant pathogen and an uncommon cause of human
infection. It has been implicated as the etiological agent
of cutaneous phaeohyphomycosis and keratitis, particularly
following colonization of traumatized tissues or in
immunocompromised patients. However, it has hardly ever been
reported in the absence of such predisposing risk factors.
Here, we report a case of keratitis with Colletotrichum
coccodes occurring in a middle- aged, immunocompetent person
without any history of trauma or co-morbidity. The isolate
was sensitive to Amphotericin B and Voriconazole, and
accordingly the patient was treated successfully with ocular
administration of Amphotericin B.},
Doi = {10.7860/jcdr/2015/10843.5529},
Key = {fds347530}
}
@article{fds308262,
Author = {Troutman, R and Kotwal, A},
Title = {Non-linear source/drain effects in amorphous-silicon
thin-film transistors},
Journal = {IEEE Transactions on Electron Devices},
Volume = {36},
Number = {11 pt 1},
Pages = {2624},
Year = {1989},
Month = {November},
Abstract = {Summary form only given. The authors discuss the effect of
space-charge-limited conduction through the a-Si layer on
n-channel staggered TFT (thin-film transistor)
current-voltage characteristics by introducing a new model
that incorporates this effect. Current density through the
a-Si film can be described by J = βφ4, where φ is the
potential from the channel to the source (or drain) contact.
Field-effect mobility in an a-Si TFT increases with gate
voltage because a greater fraction of the gate-induced
electrons is in extended tail states as the Fermi level
approaches the conduction band edge. Current flow at the
ends of the channel is roughly analogous to the transmission
line effect in shallow MOSFET source/drain diffusions, but
the effect in TFTs is highly nonlinear because of the
space-charge-limited current behavior. Experimental
current-voltage characteristics measured on a variety of
staggered TFTs closely match the simulated curves over a
wide range of terminal voltages. Differential
channel-conductance measurements of a-Si TFTs at a fixed
gate voltage reveal a peak at low drain voltage with a sharp
drop on the lower side. This behavior cannot be explained by
models using linear series impedance, but it is accurately
duplicated by the new model.},
Key = {fds308262}
}
@article{fds307678,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Novel inclusive search for the Higgs boson in the
four-lepton final state at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {7},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.86.072012},
Abstract = {An inclusive search for the standard model Higgs boson using
the four-lepton final state in proton-antiproton collisions
produced by the Tevatron at √s=1.96TeV is conducted. The
data are recorded by the CDF II detector and correspond to
an integrated luminosity of 9.7fb -1. Three distinct Higgs
decay modes, namely ZZ, WW, and ττ, are simultaneously
probed. Nine potential signal events are selected and found
to be consistent with the background expectation. We set a
95% credibility limit on the production cross section times
the branching ratio and subsequent decay to the four-lepton
final state for hypothetical Higgs boson masses between
120GeV/c2 and 300GeV/c2. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.072012},
Key = {fds307678}
}
@article{fds349182,
Author = {Kotwal, AV},
Title = {Novel methods of constraining the parton distribution
function uncertainty in the measurement of the W -boson
mass},
Journal = {Physical Review D},
Volume = {98},
Number = {3},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.98.033008},
Abstract = {The measurement of the mass of the W boson is one of the
most precise and impactful measurements to test the standard
model (SM). Following the discovery of the Higgs boson and
the measurement of its mass, all SM parameters are
sufficiently well known in order to make precise predictions
for electroweak observables such as the W boson mass. These
observables receive corrections in extensions of the SM.
Experimentally, the dominant uncertainty in the W-boson mass
measurement at hadron colliders arises due to parton
distribution functions (PDFs). We present novel in situ
methods of constraining the PDF variation and of reducing
the PDF impact on the W-mass measurement uncertainty at
hadron colliders. These methods can exploit the very
high-statistics samples of W-boson candidate events at the
LHC.},
Doi = {10.1103/PhysRevD.98.033008},
Key = {fds349182}
}
@booklet{Adams95b,
Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Breidung, H and Busza, W and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dhawan, SK and Dietrich, FS and Dougherty,
W and Dreyer, T and Eckardt, V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen,
KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Hughes, VW and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kirk, T and Kobrak, HG and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and O'Day, S and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou,
V},
Title = {Nuclear decay following deep inelastic scattering of 470 GeV
muons.},
Journal = {Physical review letters},
Volume = {74},
Number = {26},
Pages = {5198-5201},
Year = {1995},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.74.5198},
Doi = {10.1103/physrevlett.74.5198},
Key = {Adams95b}
}
@booklet{Adams98,
Author = {M. R. Adams and S. Aid and P. L. Anthony and D. A. Averill and M. D. Baker and B. R. Baller and A. Banerjee and A. A.
Bhatti and U. Bratzler and H. M. Braun and H. Breidung and W. Busza and T. J. Carroll and H. L. Clark and J. M. Conrad and R. Davisson an},
Title = {Nuclear decay following deep inelastic scattering of 470GeV
muons (vol 74, pg 5198, 1995)},
Journal = {Physical Review Letters},
Volume = {80},
Number = {9},
Pages = {2020 -- 2021},
Year = {1998},
Month = {March},
Key = {Adams98}
}
@article{fds308054,
Author = {Aaltonen, and T, and others},
Title = {Observation and mass measurement of the baryon
$Xi_b^-$},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {5},
Pages = {052002},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.052002},
Abstract = {We report the observation and measurement of the mass of the
bottom, strange baryon Xib- through the decay chain
Xib--->J/psiXi-, where J/psi-->µ+µ-, Xi--->Lambdapi-, and
Lambda-->ppi-. A signal is observed whose probability of
arising from a background fluctuation is 6.6{\AA}~10-15, or
7.7 Gaussian standard deviations. The Xib- mass is measured
to be 5792.9$\pm$2.5(stat) $\pm$1.7(syst)
MeV/c2.},
Doi = {10.1103/physrevlett.99.052002},
Key = {fds308054}
}
@article{fds355023,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
S and Balasubramanian, R and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton,
AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso,
MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
Bylund, O and Besson, N and Bethke, S and Betti, A and Bevan, AJ and Beyer,
J and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla,
JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska,
HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capua, M and Cardarelli,
R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Chytka, L and Cieri, D},
Title = {Observation and Measurement of Forward Proton Scattering in
Association with Lepton Pairs Produced via the Photon Fusion
Mechanism at ATLAS.},
Journal = {Physical review letters},
Volume = {125},
Number = {26},
Pages = {261801},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.125.261801},
Abstract = {The observation of forward proton scattering in association
with lepton pairs (e^{+}e^{-}+p or μ^{+}μ^{-}+p) produced
via photon fusion is presented. The scattered proton is
detected by the ATLAS Forward Proton spectrometer, while the
leptons are reconstructed by the central ATLAS detector.
Proton-proton collision data recorded in 2017 at a
center-of-mass energy of sqrt[s]=13 TeV are analyzed,
corresponding to an integrated luminosity of
14.6 fb^{-1}. A total of 57 (123) candidates in the
ee+p (μμ+p) final state are selected, allowing the
background-only hypothesis to be rejected with a
significance exceeding 5 standard deviations in each
channel. Proton-tagging techniques are introduced for
cross-section measurements in the fiducial detector
acceptance, corresponding to σ_{ee+p}=11.0±2.6(stat)±1.2(syst)±0.3(lumi)
and σ_{μμ+p}=7.2±1.6(stat)±0.9(syst)±0.2(lumi) fb
in the dielectron and dimuon channel, respectively.},
Doi = {10.1103/physrevlett.125.261801},
Key = {fds355023}
}
@article{fds310273,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Observation and measurement of Higgs boson decays to
WW∗with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.92.012006},
Abstract = {We report the observation of Higgs boson decays to
WW∗based on an excess over background of 6.1 standard
deviations in the dilepton final state, where the Standard
Model expectation is 5.8 standard deviations. Evidence for
the vector-boson fusion (VBF) production process is obtained
with a significance of 3.2 standard deviations. The results
are obtained from a data sample corresponding to an
integrated luminosity of 25 fb-1from √s = 7 and 8 TeV pp
collisions recorded by the ATLAS detector at the LHC. For a
Higgs boson mass of 125.36 GeV, the ratio of the measured
value to the expected value of the total production cross
section times branching fraction is 1.09+0.16-0.15(stat)+0.17-0.14(syst).
The corresponding ratios for the gluon fusion and
vector-boson fusion production mechanisms are 1.02 ±
0.19(stat)+0.22-0.18(syst) and 1.27+0.44-0.40(stat)+0.30-0.21(syst),
respectively. At √s = 8 TeV, the total production cross
sections are measured to be σ(gg→H→WW∗)=4.6±0.9(stat)+0.8-0.7(syst)
pb and σ(VBF H → WW∗)=0.51+0.17-0.15(stat)+0.13-0.08(syst)pb.
The fiducial cross section is determined for the
gluon-fusion process in exclusive final states with zero or
one associated jet.},
Doi = {10.1103/PhysRevD.92.012006},
Key = {fds310273}
}
@article{fds313601,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov,
SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger,
N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G and Conventi, F and Cooke, M and Cooper,
BD},
Title = {Observation and measurements of the production of prompt and
non-prompt [Formula: see text] mesons in association with a
[Formula: see text] boson in [Formula: see text] collisions
at [Formula: see text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {229},
Year = {2015},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3406-9},
Abstract = {The production of a [Formula: see text] boson in association
with a [Formula: see text] meson in proton-proton collisions
probes the production mechanisms of quarkonium and heavy
flavour in association with vector bosons, and allows
studies of multiple parton scattering. Using [Formula: see
text] of data collected with the ATLAS experiment at the LHC
in [Formula: see text] collisions at [Formula: see text],
the first measurement of associated [Formula: see text]
production is presented for both prompt and non-prompt
[Formula: see text] production, with both signatures having
a significance in excess of [Formula: see text]. The
inclusive production cross-sections for [Formula: see text]
boson production (analysed in [Formula: see text] or
[Formula: see text] decay modes) in association with prompt
and non-prompt [Formula: see text] are measured relative to
the inclusive production rate of [Formula: see text] bosons
in the same fiducial volume to be [Formula: see text] and
[Formula: see text] respectively. Normalised differential
production cross-section ratios are also determined as a
function of the [Formula: see text] transverse momentum. The
fraction of signal events arising from single and double
parton scattering is estimated, and a lower limit of
[Formula: see text] at [Formula: see text] confidence level
is placed on the effective cross-section regulating double
parton interactions.},
Doi = {10.1140/epjc/s10052-015-3406-9},
Key = {fds313601}
}
@article{fds308160,
Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahmed, SN and Ahn,
SH and Alexeev, GD and Alkhazov, G and Alton, A and Alverson, G and Alves,
GA and Anderson, S and Andrieu, B and Arnoud, Y and Askew, A and Asman, B and Autermann, C and Avila, C and Babukhadia, L and Bacon, TC and Baden, A and Baffioni, S and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer, P and Barnes, C and Barreto, J and Bartlett,
JF and Bassler, U and Bauer, D and Bean, A and Beauceron, S and Beaudette,
F and Begel, M and Beri, SB and Bernardi, G and Bertram, I and Besançon,
M and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Binder, M and Bischoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Bloch, D and Blumenschein, U and Boehnlein, A and Bolton, TA and Bonamy, P and Borcherding, F and Borissov, G and Bos, K and Bose, T and Boswell, C and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burdin, S and Burnett,
TH and Busato, E and Butler, JM and Bystricky, J and Canelli, F and Carvalho, W and Casey, BCK and Casey, D and Cason, NM and Castilla-Valdez, H and Chakrabarti, S and Chakraborty, D and Chan,
KM and Chandra, A and Chapin, D and Charles, F and Cheu, E and Chevalier,
L and Cho, DK and Choi, S and Chopra, S and Christiansen, T and Christofek,
L and Claes, D and Clark, AR and Clément, C and Coadou, Y and Colling, DJ and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Corcoran, M and Coss, J and Cothenet, A and Cousinou, M-C and Crépé-Renaudin, S and Cristetiu, M and Cummings, MAC and Cutts, D and da Motta, H and Davies,
B and Davies, G and Davis, GA and De, K and de Jong, P and de Jong, SJ and De
La Cruz-Burelo and E and De Oliveira Martins and C and Dean, S and Del
Signore, K and Déliot, F and Delsart, PA and Demarteau, M and Demina,
R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doidge, M and Dong, H and Doulas, S and Duflot, L and Dugad, SR and Duperrin, A and Dyer, J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Eltzroth,
JT and Elvira, VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Fein, D and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisk, HE and Fleuret, F and Fortner, M and Fox, H and Freeman, W and Fu, S and Fuess, S and Galea, CF and Gallas, E and Galyaev,
E and Gao, M and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gelé, D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Geurkov, G and Ginther, G and Goldmann, K and Golling,
T and Gómez, B and Gounder, K and Goussiou, A and Graham, G and Grannis,
PD and Greder, S and Green, JA and Greenlee, H and Greenwood, ZD and Gregores, EM and Grinstein, S and Grivaz, J-F and Groer, L and Grünendahl, S and Grünewald, MW and Gu, W and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley, NJ and Haggerty,
H and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki,
K and Hanlet, P and Harder, K and Hauptman, JM and Hauser, R and Hays, C and Hays, J and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper, R and Hou, S and Hu, Y and Huang, J and Huang, Y and Iashvili, I and Illingworth,
R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs,
K and Jenkins, A and Jesik, R and Jiang, Y and Johns, K and Johnson, M and Johnson, P and Jonckheere, A and Jonsson, P and Jöstlein, H and Juste,
A and Kado, MM and Käfer, D and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Ke, Z and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov, A and Kharchilava, A and Kharzheev, YM and Kim, KH and Klima, B and Klute, M and Kohli, JM and Kopal, M and Korablev, V and Kotcher, J and Kothari, B and Kotwal, AV and Koubarovsky, A and Kouchner, A and Kouznetsov, O and Kozelov, AV and Kozminski, J and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kurca, T and Kuznetsov, VE and Lager, S and Lahrichi, N and Landsberg, G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee, SW and Lee, WM and Leflat, A and Leggett, C and Lehner,
F and Leonidopoulos, C and Lewis, P and Li, J and Li, QZ and Li, X and Lima,
JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lobo, L and Lobodenko, A and Lokajicek, M and Lounis, A and Lu, J and Lubatti, HJ and Lucotte, A and Lueking, L and Luo, C and Lynker, M and Lyon, AL and Maciel,
AKA and Madaras, RJ and Mättig, P and Magnan, A-M and Maity, M and Mal,
PK and Malik, S and Malyshev, VL and Manankov, V and Mao, HS and Maravin,
Y and Marshall, T and Martens, M and Martin, MI and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and McMahon, T and Meder,
D and Melanson, HL and Melnitchouk, A and Meng, X and Merkin, M and Merritt, KW and Meyer, A and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mitrevski, J and Mokhov, N and Molina, J and Mondal, NK and Montgomery, HE and Moore, RW and Mostafa, M and Muanza, GS and Mulders,
M and Mutaf, YD and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding, C and Nomerotski, A and Novaes, SF and Nunnemann, T and Nurse,
E and O'Dell, V and O'Neil, DC and Oguri, V and Oliveira, N and Olivier, B and Oshima, N and Otero y Garzón and GJ and Padley, P and Papageorgiou, K and Parashar, N and Park, J and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Peters, O and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Podesta-Lerma,
PLM and Podstavkov, VM and Pope, BG and Popkov, E and Prado da Silva,
WL and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Quadt, A and Quinn, B and Rani, KJ and Rapidis, PA and Ratoff, PN and Reay,
NW and Renardy, J-F and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Royon, C and Rubinov, P and Ruchti, R and Sabirov, BM and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro, A and Savage, G and Sawyer, L and Scanlon, T and Schamberger, RD and Schellman, H and Schieferdecker, P and Schmitt, C and Schukin, A and Schwartzman, A and Schwienhorst, R and Sengupta, S and Shabalina, E and Shary, V and Shephard, WD and Shpakov, D and Sidwell, RA and Simak, V and Sirotenko,
V and Skow, D and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Song, Y and Sonnenschein, L and Sopczak, A and Sorín, V and Sosebee, M and Soustruznik, K and Souza, M and Stanton, NR and Stark, J and Steele, J and Steinbrück, G and Stevenson, K and Stolin, V and Stone, A and Stoyanova, DA and Strandberg, J and Strang, MA and Strauss, M and Ströhmer, R and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Tamburello, P and Taylor, W and Telford, P and Temple, J and Tentindo-Repond, S and Thomas, E and Thooris, B and Tomoto,
M},
Title = {Observation and properties of the X(3872) decaying to
J/psipi(+)pi(-) in pp collisions at sqrt[s]=1.96
TeV.},
Journal = {Physical review letters},
Volume = {93},
Number = {16},
Pages = {162002},
Year = {2004},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.93.162002},
Abstract = {We report the observation of the X(3872) in the
J/psipi(+)pi(-) channel, with J/psi decaying to mu(+)mu(-),
in pp collisions at sqrt[s]=1.96 TeV. Using approximately
230 pb(-1) of data collected with the Run II D0 detector, we
observe 522+/-100 X(3872) candidates. The mass difference
between the X(3872) state and the J/psi is measured to be
774.9+/-3.1(stat)+/-3.0(syst) MeV/c(2). We have investigated
the production and decay characteristics of the X(3872) and
find them to be similar to those of the psi(2S)
state.},
Doi = {10.1103/physrevlett.93.162002},
Key = {fds308160}
}
@article{fds308085,
Author = {Abulencia, and A, and others},
Title = {Observation of $B^0_s \to K^{+} K^{-}$ and Measurements of
Branching Fractions of Charmless Two-body Decays of $B^0$
and $B^0_{s}$ Mesons in $\bar{p} p$ Collisions at $\sqrt{s}$
= 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {21},
Pages = {211802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.97.211802},
Abstract = {We search for decays of the type B(s)0-->h+h[prime]- (where
h,h[prime]=K or pi) in 180 pb-1 of [overline p]p collisions
collected at the Tevatron by the upgraded Collider Detector
at Fermilab. We report the first observation of the new mode
Bs0-->K+K- with a yield of 236$\pm$32 events, corresponding
to (fs/fd)?[script B](Bs0-->K+K-)/[script
B](B0-->K+pi-)=0.46$\pm$0.08(stat)$\pm$0.07(syst), where
fs/fd is the ratio of production fractions of Bs0 and B0. We
find results in agreement with world averages for the B0
modes, and set the following new limits at 90\% C.L.:
[script B](Bs0-->K-pi+)s0-->pi+pi-)},
Doi = {10.1103/physrevlett.97.211802},
Key = {fds308085}
}
@article{fds308057,
Author = {Abulencia, and A, and others},
Title = {Observation of $WZ$ Production},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {16},
Pages = {161801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.161801},
Abstract = {We report the first observation of the associated production
of a W boson and a Z boson. This result is based on 1.1 fb-1
of integrated luminosity from p[overline p] collisions at
sqrt(s)=1.96 TeV collected with the CDF II detector at the
Fermilab Tevatron. We observe 16 WZ candidates passing our
event selection with an expected background of 2.7$\pm$0.4
events. A fit to the missing transverse energy distribution
indicates an excess of events compared to the background
expectation corresponding to a significance equivalent to 6
standard deviations. The measured cross section is
sigma(p[overline p]-->WZ)=5.0-1.6+1.8 pb, consistent with
the standard model expectation.},
Doi = {10.1103/physrevlett.98.161801},
Key = {fds308057}
}
@article{fds307876,
Author = {Aaltonen, and T, and al, E},
Title = {Observation of ${B}_{s}^{0}$\rightarrow${}J/$\psi${}{K}^{*}(892{)}^{0}$
and ${B}_{s}^{0}$\rightarrow${}J/$\psi${}{K}_{S}^{0}$
decays},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {5},
Pages = {052012},
Publisher = {American Physical Society},
Year = {2011},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.83.052012},
Abstract = {We report the first observation of two Cabibbo-suppressed
decay modes of the Bs0 meson. Using a sample of pp̄
collisions at √s=1.96TeV corresponding to 5.9fb-1 of
integrated luminosity collected with the CDF II, the
collider detector at the Fermilab Tevatron, we search for
new Bs0 decay modes in a sample of events containing
J/ψ→μ+μ - decays. We reconstruct a Bs0→J/ψK*(892)0
signal with K*(892)0→K+π-, observing a yield of 151±25
events with a statistical significance of 8.0σ. We also
reconstruct a Bs0→J/ψKS0 signal with KS0→π+π-,
observing a yield of 64±14 events with a statistical
significance of 7.2σ. From these yields, we extract the
branching ratios B(Bs0→J/ψK*(892)0)=(8. 3±3.8)×10-5 and
B(Bs0→J/ψK0)=(3.5±0.8) ×10-5, where statistical,
systematic, and fragmentation- fraction uncertainties are
included in the combined uncertainty. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.83.052012},
Key = {fds307876}
}
@article{fds307719,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and A°kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, JF and Arik, E},
Title = {Observation of a new particle in the search for the Standard
Model Higgs boson with the ATLAS detector at the
LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {716},
Number = {1},
Pages = {1-29},
Publisher = {Elsevier BV},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2012.08.020},
Abstract = {A search for the Standard Model Higgs boson in proton-proton
collisions with the ATLAS detector at the LHC is presented.
The datasets used correspond to integrated luminosities of
approximately 4.8 fb -1 collected at s=7 TeV in 2011 and 5.8
fb -1 at s=8 TeV in 2012. Individual searches in the
channels H→ZZ (*) →4ℓ, H→γγ and H→WW (*)
→eνμν in the 8 TeV data are combined with previously
published results of searches for H→ZZ (*) , WW (*) , bb-
and τ + τ - in the 7 TeV data and results from improved
analyses of the H→ZZ (*) →4ℓ and H→γγ channels in
the 7 TeV data. Clear evidence for the production of a
neutral boson with a measured mass of 126.0±0.4(stat)±0.4(sys)GeV
is presented. This observation, which has a significance of
5.9 standard deviations, corresponding to a background
fluctuation probability of 1.7×10 -9 , is compatible with
the production and decay of the Standard Model Higgs boson.
© 2012 CERN.},
Doi = {10.1016/j.physletb.2012.08.020},
Key = {fds307719}
}
@article{fds307708,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B and Clement, C and Clifft, RW},
Title = {Observation of a new χ(b) state in radiative transitions to
Υ(1S) and Υ(2S) at ATLAS.},
Journal = {Physical review letters},
Volume = {108},
Number = {15},
Pages = {152001},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.108.152001},
Abstract = {The χ(b)(nP) quarkonium states are produced in
proton-proton collisions at the Large Hadron Collider at
sqrt[s] = 7 TeV and recorded by the ATLAS detector.
Using a data sample corresponding to an integrated
luminosity of 4.4 fb(-1), these states are
reconstructed through their radiative decays to Υ(1S,2S)
with Υ → μ+ μ-. In addition to the mass peaks
corresponding to the decay modes χ(b)(1P,2P) → Υ(1S)γ,
a new structure centered at a mass of 10.530 ± 0.005(stat)
± 0.009(syst) GeV is also observed, in both the
Υ(1S)γ and Υ(2S)γ decay modes. This structure is
interpreted as the χ(b)(3P) system.},
Doi = {10.1103/physrevlett.108.152001},
Key = {fds307708}
}
@article{fds373609,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez,
O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal,
D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F},
Title = {Observation of an Excess of Dicharmonium Events in the
Four-Muon Final State with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {15},
Pages = {151902},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.151902},
Abstract = {A search is made for potential ccc[over ¯]c[over ¯]
tetraquarks decaying into a pair of charmonium states in the
four muon final state using proton-proton collision data at
sqrt[s]=13 TeV, corresponding to an integrated
luminosity of 140 fb^{-1} recorded by the ATLAS
experiment at LHC. Two decay channels, J/ψ+J/ψ→4μ and
J/ψ+ψ(2S)→4μ, are studied. Backgrounds are estimated
based on a hybrid approach involving Monte Carlo
simulations and data-driven methods. Statistically
significant excesses with respect to backgrounds dominated
by the single parton scattering are seen in the di-J/ψ
channel consistent with a narrow resonance at 6.9 GeV and a
broader structure at lower mass. A statistically significant
excess is also seen in the J/ψ+ψ(2S) channel. The fitted
masses and decay widths of the structures are
reported.},
Doi = {10.1103/physrevlett.131.151902},
Key = {fds373609}
}
@article{fds310342,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin,
M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea,
V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov,
A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG},
Title = {Observation of an excited Bc(±) meson state with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {113},
Number = {21},
Pages = {212004},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.113.212004},
Abstract = {A search for excited states of the Bc(±) meson is performed
using 4.9 fb(-1) of 7 TeV and 19.2 fb(-1) of 8 TeV
pp collision data collected by the ATLAS experiment at the
LHC. A new state is observed through its hadronic transition
to the ground state, with the latter detected in the decay
Bc(±)→J/ψπ(±). The state appears in the
m(Bc(±)π(+)π(-))-m(Bc(±))-2m(π(±)) mass difference
distribution with a significance of 5.2 standard deviations.
The mass of the observed state is 6842±4±5 MeV, where
the first error is statistical and the second is systematic.
The mass and decay of this state are consistent with
expectations for the second S-wave state of the Bc(±)
meson, Bc(±)(2S).},
Doi = {10.1103/physrevlett.113.212004},
Key = {fds310342}
}
@article{fds307602,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu,
E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee,
P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behar Harpaz and S and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Bernlochner, FU and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Chow, BKB and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou,
Y},
Title = {Observation of associated near-side and away-side long-range
correlations in sqrt[s(NN)]=5.02 TeV proton-lead collisions
with the ATLAS detector.},
Journal = {Physical review letters},
Volume = {110},
Number = {18},
Pages = {182302},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.110.182302},
Abstract = {Two-particle correlations in relative azimuthal angle (Δø)
and pseudorapidity (Δη) are measured in sqrt[s(NN)] = 5.02
TeV p+Pb collisions using the ATLAS detector at the LHC. The
measurements are performed using approximately 1 μb(-1) of
data as a function of transverse momentum (p(T)) and the
transverse energy (ΣE(T)(Pb)) summed over 3.1 < η < 4.9 in
the direction of the Pb beam. The correlation function,
constructed from charged particles, exhibits a long-range (2
< |Δ η | < 5) "near-side" (Δø ~ 0) correlation that
grows rapidly with increasing ΣE(T)(Pb). A long-range
"away-side" (Δø ~ π) correlation, obtained by subtracting
the expected contributions from recoiling dijets and other
sources estimated using events with small ΣE(T)(Pb), is
found to match the near-side correlation in magnitude, shape
(in Δη and Δø) and ΣE(T)(Pb) dependence. The resultant
Δø correlation is approximately symmetric about π/2, and
is consistent with a dominant cos2Δø modulation for all
ΣE(T)(Pb) ranges and particle p(T).},
Doi = {10.1103/physrevlett.110.182302},
Key = {fds307602}
}
@article{fds348711,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Budroni, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carrillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copie, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas,
J and Culbertson, R and Cully, JC and Cyr, D and DaRonco, S and D'Auria, S and Davies, T and D'Onofrio, M and Dagenhart, D and Barbaro, PD and Ceceo,
SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and DiTuro,
P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Foland, A and Forrester, S and Foster, GW and Franklin,
M and Freeman, JC and Frisch, HJ and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay,
C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson,
A and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Griffiths,
M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hare, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hartz, M and Hatakeyama, K and Hauser, J and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, AC and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami,
S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefevre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean,
R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martinez, M and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez,
PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nagano, A and Naganoma, J and Nahn, S and Nakano, and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Porteil, X and Poukhov, O and Pounder, N and Prokoshin, F and Pronko, A and Proudfoot, J and Ptochos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ranjan,
N and Rappoccio, S and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
R and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sánchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
I},
Title = {Observation of B s0 - B̄
s0 oscillations},
Journal = {Physical Review Letters},
Volume = {97},
Number = {24},
Pages = {242003},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevLett.97.242003},
Abstract = {We report the observation of B s0- B̄ s0 oscillations from
a time-dependent measurement of the B s0-B̄ s0 oscillation
frequency Δm s. Using a data sample of 1 fb -1 of pp
collisions at √ = 1.96 TeV collected with the CDF II
detector at the Fermilab Tevatron, we find signals of 5600
fully reconstructed hadronic B s decays, 3100 partially
reconstructed hadronic B s decays, and 61500 partially
reconstructed semileptonic B s decays. We measure the
probability as a function of proper decay time that the B s
decays with the same, or opposite, flavor as the flavor at
production, and we find a signal for B s0-B̄ s0
oscillations. The probability that random fluctuations could
produce a comparable signal is 8 × 10 -8, which exceeds 5σ
significance. We measure Δm s = 17.77 ± 0.10(stat) ±
0.07(syst) ps -1 and extract |V td/V ts| = 0.2060 ±
0.0007(Δm s) -0.0060+0.0081 (Δm d + theor). © 2006 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.97.242003},
Key = {fds348711}
}
@article{fds344671,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro,
A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cresciolo, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo,
T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez,
JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Furic,
I and Gallinaro, M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris,
N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and Gonzalez, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper,
S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer, A and Heinemann, B and Heinrich, J and Herndon, M and Hidas,
D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun,
SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato, Y and Kemp,
Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee,
YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga,
H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto,
A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse,
E and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava,
R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin,
A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton, P and Rescigno, M and Richter, S and Rimondi,
F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers,
E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz,
A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman,
D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti,
A and Sinervo, P and Sisakyan, A and Sjolin, J},
Title = {Observation of Bs0→ψ(2S) and measurement of the ratio of
branching fractions B(Bs0→ψ(2S) /B(Bs0→J/ψ)},
Journal = {Physical Review Letters},
Volume = {96},
Number = {23},
Pages = {231801},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevLett.96.231801},
Abstract = {We report the first observation of Bs0→ψ(2S) decay in
pp̄ collisions at s= 1.96 TeV using 360 pb-1 of data
collected by the CDF II detector at the Fermilab Tevatron.
We observe 20.2±5.0 and 12.3±4.1 Bs0→ψ(2S) candidates,
in ψ(2S)→μ+μ- and ψ(2S)→J/ψπ+π- decay modes,
respectively. We present a measurement of the relative
branching fraction B(Bs0→ψ(2S) /B(Bs0→J/ψ)=0.52±0.13(stat)±0.04(syst)±0.06(BR)
using the ψ(2S)→μ+μ- decay mode. © 2006 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.96.231801},
Key = {fds344671}
}
@article{fds347455,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V},
Title = {Observation of Centrality-Dependent Acoplanarity for Muon
Pairs Produced via Two-Photon Scattering in Pb+Pb Collisions
at sqrt[s_{NN}]=5.02 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {121},
Number = {21},
Pages = {212301},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.121.212301},
Abstract = {This Letter presents a measurement of γγ→μ^{+}μ^{-}
production in Pb+Pb collisions recorded by the ATLAS
detector at the Large Hadron Collider at
sqrt[s_{NN}]=5.02 TeV with an integrated luminosity of
0.49 nb^{-1}. The azimuthal angle and transverse
momentum correlations between the muons are measured as a
function of collision centrality. The muon pairs are
produced from γγ through the interaction of the large
electromagnetic fields of the nuclei. The contribution from
background sources of muon pairs is removed using a template
fit method. In peripheral collisions, the muons exhibit a
strong back-to-back correlation consistent with previous
measurements of muon pair production in ultraperipheral
collisions. The angular correlations are observed to broaden
significantly in central collisions. The modifications are
qualitatively consistent with rescattering of the muons
while passing through the hot matter produced in the
collision.},
Doi = {10.1103/physrevlett.121.212301},
Key = {fds347455}
}
@article{fds307559,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kulkarni, N and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese,
L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta,
A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra,
A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S},
Title = {Observation of D⁰-D¯⁰ mixing using the CDF II
detector.},
Journal = {Physical review letters},
Volume = {111},
Number = {23},
Pages = {231802},
Year = {2013},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.111.231802},
Abstract = {We measure the time dependence of the ratio of decay rates
for D0→K(+)π(-) to the Cabibbo-favored decay
D(0)→K(-)π(+). The charge conjugate decays are included.
A signal of 3.3×10(4) D(*+)→π(+)D(0), D(0)→K(+)π(-)
decays is obtained with D0 proper decay times between 0.75
and 10 mean D0 lifetimes. The data were recorded with the
CDF II detector at the Fermilab Tevatron and correspond to
an integrated luminosity of 9.6 fb(-1) for pp¯
collisions at √s=1.96 TeV. Assuming CP conservation,
we search for D0-D¯0 mixing and measure the mixing
parameters to be R(D)=(3.51±0.35)×10(-3),
y'=(4.3±4.3)×10(-3), and x'2=(0.08±0.18)×10(-3). We
report Bayesian probability intervals in the x'2-y' plane
and find that the significance of excluding the no-mixing
hypothesis is equivalent to 6.1 Gaussian standard
deviations, providing the second observation of D0-D¯0
mixing from a single experiment.},
Doi = {10.1103/physrevlett.111.231802},
Key = {fds307559}
}
@article{fds347181,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines,
JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi
Gupta, D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee,
S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall,
A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer,
F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, V and Buschmann, E and Bussey,
PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera
Urbán, S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace,
N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans,
R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney,
RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ},
Title = {Observation of Electroweak Production of a Same-Sign W Boson
Pair in Association with Two Jets in pp Collisions at
sqrt[s]=13 TeV with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {123},
Number = {16},
Pages = {161801},
Year = {2019},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.123.161801},
Abstract = {This Letter presents the observation and measurement of
electroweak production of a same-sign W boson pair in
association with two jets using 36.1 fb^{-1} of
proton-proton collision data recorded at a center-of-mass
energy of sqrt[s]=13 TeV by the ATLAS detector at the
Large Hadron Collider. The analysis is performed in the
detector fiducial phase-space region, defined by the
presence of two same-sign leptons, electron or muon, and at
least two jets with a large invariant mass and rapidity
difference. A total of 122 candidate events are observed for
a background expectation of 69±7 events, corresponding to
an observed signal significance of 6.5 standard deviations.
The measured fiducial signal cross section is
σ^{fid}=2.89_{-0.48}^{+0.51}(stat)_{-0.28}^{+0.29}(syst) fb.},
Doi = {10.1103/physrevlett.123.161801},
Key = {fds347181}
}
@article{fds374996,
Author = {A.V. Kotwal and the ATLAS Collaboration},
Title = {Observation of electroweak production of two jets and a
Z-boson pair},
Volume = {19},
Pages = {237–253},
Publisher = {Nature Physics},
Year = {2023},
Month = {February},
ISSN = {Nature Physics},
url = {http://dx.doi.org/https://doi.org/10.1038/s41567-022-01757-y},
Doi = {https://doi.org/10.1038/s41567-022-01757-y},
Key = {fds374996}
}
@article{fds362129,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Observation of electroweak production of two jets in
association with an isolated photon and missing transverse
momentum, and search for a Higgs boson decaying into
invisible particles at 13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {2},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09878-z},
Abstract = {This paper presents a measurement of the electroweak
production of two jets in association with a Zγ pair, with
the Z boson decaying into two neutrinos. It also presents a
search for invisible or partially invisible decays of a
Higgs boson with a mass of 125 GeV produced through
vector-boson fusion with a photon in the final state. These
results use data from LHC proton–proton collisions at s =
13 TeV collected with the ATLAS detector and corresponding
to an integrated luminosity of 139 fb - 1. The event
signature, shared by all benchmark processes considered for
the measurements and searches, is characterized by a
significant amount of unbalanced transverse momentum and a
photon in the final state, in addition to a pair of forward
jets. Electroweak Zγ production in association with two
jets is observed in this final state with a significance of
5.2 (5.1 expected) standard deviations. The measured
fiducial cross-section for this process is 1.31 ± 0.29 fb.
An observed (expected) upper limit of 0.37 (0.34-0.10+0.15)
at 95% confidence level is set on the branching ratio of a
125 GeV Higgs boson to invisible particles, assuming the
Standard Model production cross-section. The signature is
also interpreted in the context of decays of a Higgs boson
into a photon and a dark photon. An observed (expected) 95%
CL upper limit on the branching ratio for this decay is set
at 0.018 (0.017-0.005+0.007), assuming the Standard Model
production cross-section for a 125 GeV Higgs
boson.},
Doi = {10.1140/epjc/s10052-021-09878-z},
Key = {fds362129}
}
@article{fds307945,
Author = {Aaltonen, T and others},
Title = {Observation of Electroweak Single Top-Quark
Production},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {9},
Pages = {092002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.092002},
Abstract = {We report the observation of single top-quark production
using 3.2 fb-1 of pp̅ collision data with
sqrt[s]=1.96 TeV collected by the Collider Detector at
Fermilab. The significance of the observed data is 5.0
standard deviations, and the expected sensitivity for
standard model production and decay is in excess of 5.9
standard deviations. Assuming mt=175 GeV/c2, we measure
a cross section of 2.3-0.5+0.6(stat+syst) pb, extract
the CKM matrix-element value |Vtb|=0.91 ±
0.11(stat+syst) ± 0.07(theory), and set the limit
|Vtb|>0.71 at the 95% C.L.},
Doi = {10.1103/physrevlett.103.092002},
Key = {fds307945}
}
@article{fds356590,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster,
AJ},
Title = {Observation of electroweak W±Z boson pair
production in association with two jets in pp collisions at
s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {793},
Pages = {469-492},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1016/j.physletb.2019.05.012},
Abstract = {An observation of electroweak W±Z production in association
with two jets in proton–proton collisions is presented.
The data collected by the ATLAS detector at the Large Hadron
Collider in 2015 and 2016 at a centre-of-mass energy of s=13
TeV are used, corresponding to an integrated luminosity of
36.1fb−1. Events containing three identified leptons,
either electrons or muons, and two jets are selected. The
electroweak production of W±Z bosons in association with
two jets is measured with an observed significance of 5.3
standard deviations. A fiducial cross-section for
electroweak production including interference effects and
for a single leptonic decay mode is measured to be
σWZjj−EW=0.57−0.13+0.14(stat.)−0.06+0.07(syst.)fb.
Total and differential fiducial cross-sections of the sum of
W±Zjj electroweak and strong productions for several
kinematic observables are also measured.},
Doi = {10.1016/j.physletb.2019.05.012},
Key = {fds356590}
}
@article{fds307970,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey,
P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani,
M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko,
BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal,
AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan,
P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino,
CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín,
R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla
Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla,
A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer,
B},
Title = {Observation of exclusive charmonium production and
gammagamma --> micro;{+}micro;{-} in pp[over] collisions at
sqrt[s] = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {24},
Pages = {242001},
Year = {2009},
Month = {June},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.102.242001},
Abstract = {In CDF we have observed the reactions p + p[over] --> p + X
+ p[over], with X being a centrally produced J/psi, psi(2S),
or chi_{c0}, and gammagamma-->micro;{+}micro;{-} in pp[over]
collisions at sqrt[s] = 1.96 TeV. The event signature
requires two oppositely charged central muons, and either no
other particles or one additional photon detected. Exclusive
vector meson production is as expected for elastic
photoproduction, gamma + p --> J/psi(psi(2S)) + p, observed
here for the first time in hadron-hadron collisions. We also
observe exclusive chi_{c0} --> J/psi + gamma. The cross
sections dsigma/dy|_{y = 0} for J/psi, psi(2S), and chi_{c0}
are 3.92 +/- 0.25(stat) +/- 0.52(syst) nb, 0.53 +/-
0.09(stat) +/- 0.10(syst) nb, and 76 +/- 10(stat) +/-
10(syst) nb, respectively, and the continuum is consistent
with QED. We put an upper limit on the cross section for
Odderon exchange in exclusive J/psi production.},
Doi = {10.1103/physrevlett.102.242001},
Key = {fds307970}
}
@article{fds307713,
Author = {Aaltonen, T and others},
Title = {Observation of Exclusive Charmonium Production and
γγ→μ+μ- in pp̅ Collisions at sqrt[s] =1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {24},
Pages = {242001},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.108.081801},
Abstract = {In CDF we have observed the reactions p+p̅ →p+X+p̅ ,
with X being a centrally produced J/ψ, ψ(2S), or χc0, and
γγ→μ+μ- in pp̅ collisions at sqrt[s]=1.96 TeV.
The event signature requires two oppositely charged central
muons, and either no other particles or one additional
photon detected. Exclusive vector meson production is as
expected for elastic photoproduction, γ+p→J/ψ(ψ(2S))+p,
observed here for the first time in hadron-hadron
collisions. We also observe exclusive χc0→J/ψ+γ. The
cross sections dσ / dy|y=0 for J/ψ, ψ(2S), and χc0 are
3.92 ± 0.25(stat) ± 0.52(syst) nb, 0.53
± 0.09(stat) ± 0.10(syst) nb, and 76
± 10(stat) ± 10(syst) nb, respectively,
and the continuum is consistent with QED. We put an upper
limit on the cross section for Odderon exchange in exclusive
J/ψ production.},
Doi = {10.1103/physrevlett.108.081801},
Key = {fds307713}
}
@article{fds308061,
Author = {Abulencia, and A, and others},
Title = {Observation of exclusive electron positron production in
hadron hadron collisions},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {11},
Pages = {112001},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.112001},
Abstract = {We present the first observation of exclusive e+e-
production in hadron-hadron collisions, using p[overline p]
collision data at sqrt(s)=1.96 TeV taken by the run II
Collider Detector at Fermilab, and corresponding to an
integrated luminosity of 532 pb-1. We require the absence of
any particle signatures in the detector except for an
electron and a positron candidate, each with transverse
energy ET>5 GeV and pseudorapidity |eta|p+e+e-+[overline p]
through two-photon exchange. The measured cross section is
1.6-0.3+0.5(stat)$\pm$0.3(syst) pb. This agrees with the
theoretical prediction of 1.71$\pm$0.01 pb.},
Doi = {10.1103/physrevlett.98.112001},
Key = {fds308061}
}
@article{fds372390,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA},
Title = {Observation of four-top-quark production in the multilepton
final state with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11573-0},
Abstract = {This paper presents the observation of four-top-quark (tt¯
tt¯) production in proton-proton collisions at the LHC. The
analysis is performed using an integrated luminosity of 140
fb - 1 at a centre-of-mass energy of 13 TeV collected using
the ATLAS detector. Events containing two leptons with the
same electric charge or at least three leptons (electrons or
muons) are selected. Event kinematics are used to separate
signal from background through a multivariate discriminant,
and dedicated control regions are used to constrain the
dominant backgrounds. The observed (expected) significance
of the measured tt¯ tt¯ signal with respect to the
standard model (SM) background-only hypothesis is 6.1 (4.3)
standard deviations. The tt¯ tt¯ production cross section
is measured to be 22.5-5.5+6.6 fb, consistent with the SM
prediction of 12.0 ± 2.4 fb within 1.8 standard deviations.
Data are also used to set limits on the three-top-quark
production cross section, being an irreducible background
not measured previously, and to constrain the top-Higgs
Yukawa coupling and effective field theory operator
coefficients that affect tt¯ tt¯ production.},
Doi = {10.1140/epjc/s10052-023-11573-0},
Key = {fds372390}
}
@article{fds372120,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V},
Title = {Observation of gauge boson joint-polarisation states in
W±Z production from pp collisions at s=13 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.137895},
Abstract = {Measurements of joint-polarisation states of W and Z gauge
bosons in W±Z production are presented. The data set used
corresponds to an integrated luminosity of 139 fb−1 of
proton–proton collisions at a centre-of-mass energy of 13
TeV recorded by the ATLAS detector at the CERN Large Hadron
Collider. The W±Z candidate events are reconstructed using
leptonic decay modes of the gauge bosons into electrons and
muons. The simultaneous pair-production of longitudinally
polarised vector bosons is measured for the first time with
a significance of 7.1 standard deviations. The measured
joint helicity fractions integrated over the fiducial region
are f00=0.067±0.010, f0T=0.110±0.029, fT0=0.179±0.023 and
fTT=0.644±0.032, in agreement with the next-to-leading-order
Standard Model predictions. Individual helicity fractions of
the W and Z bosons are also measured and found to be
consistent with joint helicity fractions within the expected
amounts of correlation. Both the joint and individual
helicity fractions are also measured separately in W+Z and
W−Z events. Inclusive and differential cross sections for
several kinematic observables sensitive to polarisation are
presented.},
Doi = {10.1016/j.physletb.2023.137895},
Key = {fds372120}
}
@article{fds356661,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Observation of Higgs boson production in association with a
top quark pair at the LHC with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {784},
Pages = {173-191},
Year = {2018},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2018.07.035},
Abstract = {The observation of Higgs boson production in association
with a top quark pair (tt¯H), based on the analysis of
proton–proton collision data at a centre-of-mass energy of
13 TeV recorded with the ATLAS detector at the Large Hadron
Collider, is presented. Using data corresponding to
integrated luminosities of up to 79.8 fb−1, and
considering Higgs boson decays into bb¯, WW⁎, τ+τ−,
γγ, and ZZ⁎, the observed significance is 5.8 standard
deviations, compared to an expectation of 4.9 standard
deviations. Combined with the tt¯H searches using a dataset
corresponding to integrated luminosities of 4.5 fb−1 at 7
TeV and 20.3 fb−1 at 8 TeV, the observed (expected)
significance is 6.3 (5.1) standard deviations. Assuming
Standard Model branching fractions, the total tt¯H
production cross section at 13 TeV is measured to be 670 ±
90 (stat.) −100+110 (syst.) fb, in agreement with the
Standard Model prediction.},
Doi = {10.1016/j.physletb.2018.07.035},
Key = {fds356661}
}
@article{fds356638,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S},
Title = {Observation of H→bb¯ decays and VH production with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {786},
Pages = {59-86},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2018.09.013},
Abstract = {A search for the decay of the Standard Model Higgs boson
into a bb¯ pair when produced in association with a W or Z
boson is performed with the ATLAS detector. The data,
corresponding to an integrated luminosity of 79.8fb−1 were
collected in proton–proton collisions during Run 2 of the
Large Hadron Collider at a centre-of-mass energy of 13TeV.
For a Higgs boson mass of 125GeV, an excess of events over
the expected background from other Standard Model processes
is found with an observed (expected) significance of 4.9
(4.3) standard deviations. A combination with the results
from other searches in Run 1 and in Run 2 for the Higgs
boson in the bb¯ decay mode is performed, which yields an
observed (expected) significance of 5.4 (5.5) standard
deviations, thus providing direct observation of the Higgs
boson decay into b-quarks. The ratio of the measured event
yield for a Higgs boson decaying into bb¯ to the Standard
Model expectation is 1.01±0.12(stat.)−0.15+0.16(syst.).
Additionally, a combination of Run 2 results searching for
the Higgs boson produced in association with a vector boson
yields an observed (expected) significance of 5.3 (4.8)
standard deviations.},
Doi = {10.1016/j.physletb.2018.09.013},
Key = {fds356638}
}
@article{fds347182,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O and Arnold, H and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Avramidou,
R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baca, MJ and Bachacou,
H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura,
AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barsov, S and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Berry, T and Berta, P and Bertella, C and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bitadze, A and Bittrich, C and Bjørke, K and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burr, JTP and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, FC and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carter, JWS and Casado, MP and Casha, AF and Casper,
DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, SK and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen,
C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu, MC and Chu, X and Chudoba, J},
Title = {Observation of Light-by-Light Scattering in Ultraperipheral
Pb+Pb Collisions with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {123},
Number = {5},
Pages = {052001},
Year = {2019},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.123.052001},
Abstract = {This Letter describes the observation of the light-by-light
scattering process, γγ→γγ, in Pb+Pb collisions at
sqrt[s_{NN}]=5.02 TeV. The analysis is conducted using
a data sample corresponding to an integrated luminosity of
1.73 nb^{-1}, collected in November 2018 by the ATLAS
experiment at the LHC. Light-by-light scattering candidates
are selected in events with two photons produced
exclusively, each with transverse energy
E_{T}^{γ}>3 GeV and pseudorapidity |η_{γ}|<2.4,
diphoton invariant mass above 6 GeV, and small diphoton
transverse momentum and acoplanarity. After applying all
selection criteria, 59 candidate events are observed for a
background expectation of 12±3 events. The observed excess
of events over the expected background has a significance of
8.2 standard deviations. The measured fiducial cross section
is 78±13(stat)±7(syst)±3(lumi) nb.},
Doi = {10.1103/physrevlett.123.052001},
Key = {fds347182}
}
@article{fds316844,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo,
T},
Title = {Observation of Long-Range Elliptic Azimuthal Anisotropies in
sqrt[s]=13 and 2.76 TeV pp Collisions with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {116},
Number = {17},
Pages = {172301},
Year = {2016},
Month = {April},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.116.172301},
Abstract = {ATLAS has measured two-particle correlations as a function
of the relative azimuthal angle, Δϕ, and pseudorapidity,
Δη, in sqrt[s]=13 and 2.76 TeV pp collisions at the LHC
using charged particles measured in the pseudorapidity
interval |η|<2.5. The correlation functions evaluated in
different intervals of measured charged-particle
multiplicity show a multiplicity-dependent enhancement at
Δϕ∼0 that extends over a wide range of Δη, which has
been referred to as the "ridge." Per-trigger-particle
yields, Y(Δϕ), are measured over 2<|Δη|<5. For both
collision energies, the Y(Δϕ) distribution in all
multiplicity intervals is found to be consistent with a
linear combination of the per-trigger-particle yields
measured in collisions with less than 20 reconstructed
tracks, and a constant combinatoric contribution modulated
by cos(2Δϕ). The fitted Fourier coefficient, v_{2,2},
exhibits factorization, suggesting that the ridge results
from per-event cos(2ϕ) modulation of the single-particle
distribution with Fourier coefficients v_{2}. The v_{2}
values are presented as a function of multiplicity and
transverse momentum. They are found to be approximately
constant as a function of multiplicity and to have a p_{T}
dependence similar to that measured in p+Pb and Pb+Pb
collisions. The v_{2} values in the 13 and 2.76 TeV data
are consistent within uncertainties. These results suggest
that the ridge in pp collisions arises from the same or
similar underlying physics as observed in p+Pb collisions,
and that the dynamics responsible for the ridge has no
strong sqrt[s] dependence.},
Doi = {10.1103/physrevlett.116.172301},
Key = {fds316844}
}
@article{fds307948,
Author = {Aaltonen, T and others},
Title = {Observation of New Charmless Decays of Bottom
Hadrons},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {3},
Pages = {031801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.031801},
Abstract = {We search for new charmless decays of neutral b hadrons to
pairs of charged hadrons, using 1 fb-1 of data
collected by the CDF II detector at the Fermilab Tevatron.
We report the first observation of the Bs0→K-π+ decay and
measure B(Bs0→K-π+)=(5.0 ± 0.7(stat) ±
0.8(syst))×10-6. We also report the first observation of
charmless b-baryon decays, and measure B(Λb0→pπ-)=(3.5
± 0.6(stat) ± 0.9(syst))×10-6 and
B(Λb0→pK-)=(5.6 ± 0.8(stat) ±
1.5(syst))×10-6. No evidence is found for other modes, and
we set the limit B(Bs0→π+π-)<1.2×10-6 at 90%
C.L.},
Doi = {10.1103/physrevlett.103.031801},
Key = {fds307948}
}
@article{fds307532,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de Barbaro, P and de Jong, SJ and De La
Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov, SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto, F and Di Canto and A and Di Ruzza,
B and Diehl, HT and Diesburg, M and Ding, PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti,
A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, VN and Farrington, S and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov,
V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Grinstein, S and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim,
YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich, I and Knoepfel,
K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr,
T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon,
K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li,
H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour,
J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega,
J and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta,
A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed,
S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett,
J and Neu, C and Neustroev, P},
Title = {Observation of s-channel production of single top quarks at
the Tevatron.},
Journal = {Physical review letters},
Volume = {112},
Number = {23},
Pages = {231803},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.112.231803},
Abstract = {We report the first observation of single-top-quark
production in the s channel through the combination of the
CDF and D0 measurements of the cross section in
proton-antiproton collisions at a center-of-mass energy of
1.96 TeV. The data correspond to total integrated
luminosities of up to 9.7 fb(-1) per experiment. The
measured cross section is σ(s) = 1.29(-0.24)(+0.26) pb. The
probability of observing a statistical fluctuation of the
background to a cross section of the observed size or larger
is 1.8 × 10(-10), corresponding to a significance of 6.3
standard deviations for the presence of an s-channel
contribution to the production of single-top
quarks.},
Doi = {10.1103/physrevlett.112.231803},
Key = {fds307532}
}
@article{fds307921,
Author = {Aaltonen, and T, and others},
Title = {Observation of single top quark production and measurement
of |$V_{tb}|$ with CDF},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {11},
Pages = {112005},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.82.112005},
Abstract = {We report the observation of electroweak single top quark
production in 3.2fb⊃-1 of pp̄ collision data collected by
the Collider Detector at Fermilab at √s=1.96TeV. Candidate
events in the W+jets topology with a leptonically decaying W
boson are classified as signal-like by four parallel
analyses based on likelihood functions, matrix elements,
neural networks, and boosted decision trees. These results
are combined using a super discriminant analysis based on
genetically evolved neural networks in order to improve the
sensitivity. This combined result is further combined with
that of a search for a single top quark signal in an
orthogonal sample of events with missing transverse energy
plus jets and no charged lepton. We observe a signal
consistent with the standard model prediction but
inconsistent with the background-only model by 5.0 standard
deviations, with a median expected sensitivity in excess of
5.9 standard deviations. We measure a production cross
section of 2.3-0.5+0.6(stat+sys)pb, extract the value of the
Cabibbo-Kobayashi-Maskawa matrix element |Vtb|=0.91-0.11+0.
11(stat+sys)±0.07(theory), and set a lower limit |Vtb|>0.71
at the 95%C.L., assuming mt=175GeV/c2.},
Doi = {10.1103/PhysRevD.82.112005},
Key = {fds307921}
}
@article{fds374211,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira,
MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos,
P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat,
A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley,
JR and Batool, B and Battaglia, M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer,
JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi,
G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov,
VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden
Madden, WD and Brendlinger, K and Brener, R and Brenner, L and Brenner,
R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de
Renstrom, PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov,
O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson,
SE},
Title = {Observation of Single-Top-Quark Production in Association
with a Photon Using the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {18},
Pages = {181901},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.131.181901},
Abstract = {This Letter reports the observation of single top quarks
produced together with a photon, which directly probes the
electroweak coupling of the top quark. The analysis uses
139 fb^{-1} of 13 TeV proton-proton collision data
collected with the ATLAS detector at the Large Hadron
Collider. Requiring a photon with transverse momentum larger
than 20 GeV and within the detector acceptance, the
fiducial cross section is measured to be
688±23(stat) _{-71}^{+75}(syst) fb, to be compared
with the standard model prediction of 515_{-42}^{+36} fb
at next-to-leading order in QCD.},
Doi = {10.1103/physrevlett.131.181901},
Key = {fds374211}
}
@article{fds307700,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker,
C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
W},
Title = {Observation of spin correlation in tt¯ events from pp
collisions at √s=7 TeV using the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {108},
Number = {21},
Pages = {212001},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.212001},
Abstract = {A measurement of spin correlation in tt[over ¯] production
is reported using data collected with the ATLAS detector at
the LHC, corresponding to an integrated luminosity of 2.1
fb(-1). Candidate events are selected in the dilepton
topology with large missing transverse energy and at least
two jets. The difference in azimuthal angle between the two
charged leptons in the laboratory frame is used to extract
the correlation between the top and antitop quark spins. In
the helicity basis the measured degree of correlation
corresponds to A(helicity)=0.40(-0.08)(+0.09), in agreement
with the next-to-leading-order standard model prediction.
The hypothesis of zero spin correlation is excluded at 5.1
standard deviations.},
Doi = {10.1103/physrevlett.108.212001},
Key = {fds307700}
}
@article{fds307839,
Author = {Aaltonen, and T, and al, E},
Title = {Observation of the $\Xi_{b}^{0}$ Baryon},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {10},
Pages = {102001},
Publisher = {American Physical Society},
Year = {2011},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.102001},
Abstract = {The observation of the bottom, strange baryon Ξ(b)(0)
through the decay chain Ξ(b)(0)→Ξ(c)(+)π-, where
ΞΞ(c)(+)→Ξ- π+ π+, Ξ-→Λπ-, and Λ→pπ-, is
reported by using data corresponding to an integrated
luminosity of 4.2 fb(-1) from pp collisions at square
root(s)=1.96 TeV recorded with the Collider Detector at
Fermilab. A signal of 25.3(-5.4)(+5.6) candidates is
observed whose probability of arising from a background
fluctuation is 3.6×10(-12), corresponding to 6.8 gaussian
standard deviations. The Ξ(b)(0) mass is measured to be
5787.8±5.0(stat)±1.3(syst) MeV/c2. In addition, the
Ξ(b)- baryon is observed through the process
Ξ(b)-→Ξ(c)(0)π-, where Ξ(c)(0)→Ξ- π+, Ξ-→Λπ-,
and Λ→pπ-.},
Doi = {10.1103/PhysRevLett.107.102001},
Key = {fds307839}
}
@article{fds351556,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
Title = {Observation of the associated production of a top quark and
a Z boson in pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {7},
Year = {2020},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2020)124},
Abstract = {Single top-quark production in association with a Z boson,
where the Z boson decays to a pair of charged leptons, is
measured in the trilepton channel. The proton-proton
collision data collected by the ATLAS experiment from 2015
to 2018 at a centre-of-mass energy of 13 TeV are used,
corresponding to an integrated luminosity of 139 fb−1.
Events containing three isolated charged leptons (electrons
or muons) and two or three jets, one of which is identified
as containing a b-hadron, are selected. The main backgrounds
are from tt¯ Z and diboson production. Neural networks are
used to improve the background rejection and extract the
signal. The measured cross-section for tℓ+ℓ−q
production, including non-resonant dilepton pairs with
mℓ+ℓ−> 30 GeV, is 97 ± 13 (stat.) ± 7 (syst.) fb,
consistent with the Standard Model prediction. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP07(2020)124},
Key = {fds351556}
}
@article{fds307833,
Author = {Aaltonen, TEA},
Title = {Observation of the Baryonic Flavor-Changing Neutral Current
Decay $\Lambda_{b}^{0}\rightarrow\Lambda\mu^{+}\mu^{-}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {20},
Pages = {201802},
Publisher = {American Physical Society},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.201802},
Abstract = {We report the first observation of the baryonic
flavor-changing neutral current decay Λ(b)(0)→Λμ(+)μ(-)
with 24 signal events and a statistical significance of 5.8
Gaussian standard deviations. This measurement uses a pp
collisions data sample corresponding to 6.8 fb(-1) at √s =
1.96 TeV collected by the CDF II detector at the Tevatron
collider. The total and differential branching ratios for
Λ(b)(0)→Λμ(+)μ(-) are measured. We find
B(Λ(b)(0)→Λμ(+)μ(-))=[1.73 ± 0.42(stat) ± (syst)] ×
10(-6). We also report the first measurement of the
differential branching ratio of B(s)(0)→ϕμ(+)μ(-),
using 49 signal events. In addition, we report branching
ratios for B(+)→K(+)μ(+)μ(-), B(0)→K(0)μ(+)μ(-), and
B→K(*)(892)μ(+)μ(-) decays.},
Doi = {10.1103/PhysRevLett.107.201802},
Key = {fds307833}
}
@article{fds361694,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and Barbaro, PD and Cecco, SD and Deisher, A and Lentdecker, GD and Lorenzo,
GD and Dell'Orso, M and Demortier, L and Deng, J and Deninno, M and Pedis,
DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare,
M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun,
SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato,
Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson,
B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus, J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone,
S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, RS and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and MacK, P and MacQueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli,
F and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Griso,
SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic,
V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori,
L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó,
O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ},
Title = {Observation of the decay Bc±→J/ψπ± and measurement of
the Bc± mass},
Journal = {Physical Review Letters},
Volume = {100},
Number = {18},
Pages = {182002},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevLett.100.182002},
Abstract = {The Bc± meson is observed through the decay Bc±→J/
ψπ±, in data corresponding to an integrated luminosity of
2.4fb-1 recorded by the Collider Detector at Fermilab II
detector at the Fermilab Tevatron. A signal of 108±15
candidates is observed, with a significance that exceeds
8σ. The mass of the Bc± meson is measured to be
6275.6±2.9(stat)±2.5(syst)MeV/c2. © 2008 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.100.182002},
Key = {fds361694}
}
@article{fds308066,
Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Behari,
S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and DaRonco, S and Datta, M and D'Auria, S and Davies, T and Dagenhart, D and de Barbaro, P and De
Cecco, S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'Orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Dörr,
C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani,
M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson,
C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl,
D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marginean,
R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel,
P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles,
J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher,
G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore,
R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou,
A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov,
A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar,
S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima,
M and Shochet, M and Shon, Y},
Title = {Observation of the Heavy Baryons Sigma b and Sigma
b*.},
Journal = {Physical review letters},
Volume = {99},
Number = {20},
Pages = {202001},
Year = {2007},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.99.202001},
Abstract = {We report an observation of new bottom baryons produced in
pp collisions at the Tevatron. Using 1.1 fb(-1) of data
collected by the CDF II detector, we observe four Lambda b 0
pi+/- resonances in the fully reconstructed decay mode
Lambda b 0-->Lambda c + pi-, where Lambda c+-->pK* pi+. We
interpret these states as the Sigma b(*)+/- baryons and
measure the following masses: m Sigma b+=5807.8 -2.2
+2.0(stat.)+/-1.7(syst.) MeV/c2, m Sigma b-
=5815.2+/-1.0(stat.)+/-1.7(syst.) MeV/c2, and m(Sigma
b*)-m(Sigma b)=21.2-1.9 +2.0(stat.)-0.3+0.4(syst.)
MeV/c2.},
Doi = {10.1103/physrevlett.99.202001},
Key = {fds308066}
}
@article{fds308164,
Author = {Acosta, D and Affolder, T and Ahn, MH and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Bailey, S and Barbaro-Galtieri, A and Barker, G and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bell, WH and Bellettini,
G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov,
S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett,
K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura,
P and Campanelli, M and Campbell, M and Canepa, A and Carlsmith, D and Carron, S and Carosi, R and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen,
C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chu, ML and Chung, JY and Chung,
WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, MN and Connolly, A and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cranshaw, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and DaRonco, S and D'Auria, S and Barbaro, PD and Cecco,
SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers,
S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann, JR and Doksus, P and Dominguez, A and Donati,
S and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Frisch, H and Fujii, Y and Furic, I and Gaijar, A and Gallas, A and Gallinaro, M and Galyardt, J and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, DW and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hall, C and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke,
M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman,
KD and Holloway, A and Hou, S and Houlden, MA and Huang, Y and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
H and Jones, M and Jun, SY and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim,
TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov,
K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer,
A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Leonardo, N and Leone, S and Lewis,
JD and Li, K and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loken, J and Loreti,
M and Loverre, P and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, A and Martin, M and Martin, V and Martinez, M and Maruyama, T and Matsunaga, H and Mattson,
M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Menzemer, S and Menzione, A and Merkel,
P and Mesropian, C and Messina, A and Meyer, A and Miao, T and Miladinovic,
N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mishina, M and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Moore, R and Morello, M and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Oesterberg, K and Ogawa, T and Oh, S and Oh, YD and Ohsugi, T and Oishi, R and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari,
F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
H and Reichold, A and Rekovic, V and Renton, P and Rescigno, M and Rimondi,
F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and Denis, RS and Sakumoto, WK and Saltzberg, D and Sanchez, C and Sansoni,
A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro,
A and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shon, Y and Sidoti, A and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Somalwar, SV and Spalding, J and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Squillacioti, P and Stadie, H and Stelzer, B and Stelzer-Chilton, O and Strologas, J and Stuart, D and Sukhanov, A and Sumorok,
K},
Title = {Observation of the narrow state X(3872) →
J/ψπ+π- in p̄p collisions at √s
= 1.96 TeV},
Journal = {Physical Review Letters},
Volume = {93},
Number = {7},
Pages = {072001-1-072001-6},
Year = {2004},
url = {http://dx.doi.org/10.1103/PhysRevLett.93.072001},
Abstract = {The observation of a state consistent with X(3872) decaying
into J/ψπ+π- was reported. The X(3872) mass was measured
to be 3871.3±0.7(stat)±0.4(syst)MeV/c2 from a sample of
730±90 candidates. The observed width was consistent with
the detector resolution. The results were found to be
converging well with the measurements by the Belle
Collaboration using b± decays.},
Doi = {10.1103/PhysRevLett.93.072001},
Key = {fds308164}
}
@article{fds307628,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chou, JP and Chokheli,
D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza,
B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Funakoshi, Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hopkins, W and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leone, S and Lewis, JD and Limosani, A and Lipeles,
E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys,
J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty,
R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki,
D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore,
R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia,
E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro,
A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi,
G and Wagner, P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams,
HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers,
S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato,
D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Observation of the production of a W boson in association
with a single charm quark.},
Journal = {Physical review letters},
Volume = {110},
Number = {7},
Pages = {071801},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.110.071801},
Abstract = {The first observation of the production of a W boson with a
single charm quark (c) jet in pp[over ¯] collisions at
√s=1.96 TeV is reported. The analysis uses data
corresponding to 4.3 fb(-1), recorded with the CDF II
detector at the Fermilab Tevatron. Charm quark candidates
are selected through the identification of an electron or
muon from charm-hadron semileptonic decay within a hadronic
jet, and a Wc signal is observed with a significance of 5.7
standard deviations. The production cross section
σ(Wc)(p(Tc)>20 GeV/c,|η(c)|<1.5)×B(W→ℓν) is
measured to be 13.6(-3.1)(+3.4) pb and is in agreement
with theoretical expectations. From this result the
magnitude of the quark-mixing matrix element V(cs) is
derived, |V(cs)|=1.08±0.16 along with a lower limit of
|V(cs)|>0.71 at the 95% confidence level, assuming that the
Wc production through c to s quark coupling is
dominant.},
Doi = {10.1103/physrevlett.110.071801},
Key = {fds307628}
}
@article{fds356741,
Author = {Aaltonen, T and Alvarez Gonzálezv and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Braua, B and Brigliadori, L and Brisuda,
A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell,
M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, CY and Chertok, M and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway,
J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and Ascenzo, N},
Title = {Observation of the y (4 1 4 0) structure in the J/mass
spectrum in B ±±→K ± decays},
Journal = {Modern Physics Letters A},
Volume = {32},
Number = {26},
Year = {2017},
Month = {August},
url = {http://dx.doi.org/10.1142/S0217732317501395},
Abstract = {The observation of the Y (4140) structure in B± →
J/ΨφK± decays produced in pp collisions at √ s = 1.96
TeV is reported with a statistical significance greater than
5 standard deviations. A fit to the J/Ψφ mass spectrum is
performed assuming the presence of a Breit-Wigner resonance.
The fit yields a signal of 19 ± 6 (stat) ± 3 (syst)
resonance events, and resonance mass and width of 4143.4+2.9
-3.0 (stat)±0.6 (syst) MeV/c2 and 15.3+10.4 -6.1
(stat)±2.5 (syst) MeV/c2, respectively. The parameters of
this resonancelike structure are consistent with values
reported from an earlier CDF analysis.},
Doi = {10.1142/S0217732317501395},
Key = {fds356741}
}
@article{fds373610,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron
Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram,
IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Bisceglie,
E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden
Madden, WD and Brendlinger, K and Brener, R and Brenner, L and Brenner,
R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de
Renstrom, PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov,
O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro,
V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ and Clavijo
Columbie, JM},
Title = {Observation of the γγ→ττ Process in Pb+Pb Collisions
and Constraints on the τ-Lepton Anomalous Magnetic Moment
with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {15},
Pages = {151802},
Year = {2023},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.131.151802},
Abstract = {This Letter reports the observation of τ-lepton-pair
production in ultraperipheral lead-lead collisions
Pb+Pb→Pb(γγ→ττ)Pb and constraints on the τ-lepton
anomalous magnetic moment a_{τ}. The dataset corresponds to
an integrated luminosity of 1.44 nb^{-1} of LHC Pb+Pb
collisions at sqrt[s_{NN}]=5.02 TeV recorded by the
ATLAS experiment in 2018. Selected events contain one muon
from a τ-lepton decay, an electron or charged-particle
track(s) from the other τ-lepton decay, little additional
central-detector activity, and no forward neutrons. The
γγ→ττ process is observed in Pb+Pb collisions with a
significance exceeding 5 standard deviations and a signal
strength of μ_{ττ}=1.03_{-0.05}^{+0.06} assuming the
standard model value for a_{τ}. To measure a_{τ}, a
template fit to the muon transverse-momentum distribution
from τ-lepton candidates is performed, using a dimuon
(γγ→μμ) control sample to constrain systematic
uncertainties. The observed 95% confidence-level interval
for a_{τ} is -0.057<a_{τ}<0.024.},
Doi = {10.1103/physrevlett.131.151802},
Key = {fds373610}
}
@article{fds307989,
Author = {Aaltonen, T and others},
Title = {Observation of the Ωb- baryon and measurement of the
properties of the Ξb- and Ωb- baryons},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {7},
Pages = {072003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.072003},
Abstract = {We report the observation of the bottom, doubly-strange
baryon Ωb- through the decay chain Ωb-→J/ψΩ-, where
J/ψ→μ+μ-, Ω-→ΛK-, and Λ→pπ-, using
4.2 fb-1 of data from pp̅ collisions at
sqrt[s]=1.96 TeV, and recorded with the Collider
Detector at Fermilab. A signal is observed whose probability
of arising from a background fluctuation is 4.0×10-8, or
5.5 Gaussian standard deviations. The Ωb- mass is measured
to be 6054.4 ± 6.8(stat) ±
0.9(syst) MeV/c2. The lifetime of the Ωb- baryon is
measured to be 1.13-0.40+0.53(stat) ±
0.02(syst) ps. In addition, for the Ξb- baryon we
measure a mass of 5790.9 ± 2.6(stat) ±
0.8(syst) MeV/c2 and a lifetime of 1.56-0.25+0.27(stat)
± 0.02(syst) ps. Under the assumption that the
Ξb- and Ωb- are produced with similar kinematic
distributions to the Λb0 baryon, we find
σ(Ξb-)B(Ξb-→J/ψΞ-) / σ(Λb0)B(Λb0→J/ψΛ)=0.167-0.025+0.037(stat)
± 0.012(syst) and σ(Ωb-)B(Ωb-→J/ψΩ-) /
σ(Λb0)B(Λb0→J/ψΛ)=0.045-0.012+0.017(stat) ±
0.004(syst) for baryons produced with transverse momentum in
the range of 6--20 GeV/c.},
Doi = {10.1103/PhysRevD.80.072003},
Key = {fds307989}
}
@article{fds310294,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Observation of top-quark pair production in association with
a photon and measurement of the t t ¯ γ production cross
section in pp collisions at √s =7 TeV using the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.91.072007},
Abstract = {A search is performed for top-quark pairs (tt¯) produced
together with a photon (γ) with transverse energy greater
than 20 GeV using a sample of tt¯ candidate events in final
states with jets, missing transverse momentum, and one
isolated electron or muon. The data set used corresponds to
an integrated luminosity of 4.59 fb-1 of proton-proton
collisions at a center-of-mass energy of 7 TeV recorded by
the ATLAS detector at the CERN Large Hadron Collider. In
total, 140 and 222 tt¯γ candidate events are observed in
the electron and muon channels, to be compared to the
expectation of 79±26 and 120±39 non-tt¯γ background
events, respectively. The production of tt¯γ events is
observed with a significance of 5.3 standard deviations away
from the null hypothesis. The tt¯γ production cross
section times the branching ratio (BR) of the single-lepton
decay channel is measured in a fiducial kinematic region
within the ATLAS acceptance. The measured value is
σtt¯γfid×BR=63±8(stat)-13+17(syst)±1(lumi) fb per
lepton flavor, in good agreement with the leading-order
theoretical calculation normalized to the
next-to-leading-order theoretical prediction of 48±10
fb.},
Doi = {10.1103/PhysRevD.91.072007},
Key = {fds310294}
}
@article{fds366921,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler,
A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai,
K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avner, G and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baroncelli,
A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos,
P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat,
A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley,
JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli,
M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde,
B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks,
WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko,
D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler,
JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez,
CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron,
S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
TM and Casadei, D and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen,
H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark, A and Clark, PJ and Clavijo
Columbie, JM and Clawson, SE and Clement, C and Clissa, L and Coadou,
Y},
Title = {Observation of WWW Production in pp Collisions at
sqrt[s]=13 TeV with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {129},
Number = {6},
Pages = {061803},
Year = {2022},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.129.061803},
Abstract = {This Letter reports the observation of WWW production and a
measurement of its cross section using 139 fb^{-1} of
proton-proton collision data recorded at a center-of-mass
energy of 13 TeV by the ATLAS detector at the Large Hadron
Collider. Events with two same-sign leptons (electrons or
muons) and at least two jets, as well as events with three
charged leptons, are selected. A multivariate technique is
then used to discriminate between signal and background
events. Events from WWW production are observed with a
significance of 8.0 standard deviations, where the
expectation is 5.4 standard deviations. The inclusive WWW
production cross section is measured to be
820±100 (stat)±80 (syst) fb, approximately 2.6
standard deviations from the predicted cross section of
511±18 fb calculated at next-to-leading-order QCD and
leading-order electroweak accuracy.},
Doi = {10.1103/physrevlett.129.061803},
Key = {fds366921}
}
@article{fds375334,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A},
Title = {Observation of WZγ Production in pp Collisions at
sqrt[s]=13 TeV with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {132},
Number = {2},
Pages = {021802},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.132.021802},
Abstract = {This Letter reports the observation of WZγ production and a
measurement of its cross section using 140.1±1.2 fb^{-1}
of proton-proton collision data recorded at a center-of-mass
energy of 13 TeV by the ATLAS detector at the Large Hadron
Collider. The WZγ production cross section, with both the W
and Z bosons decaying leptonically, pp→WZγ→ℓ^{'}^{±}νℓ^{+}ℓ^{-}γ
(ℓ^{(^{'})}=e, μ), is measured in a fiducial phase-space
region defined such that the leptons and the photon have
high transverse momentum and the photon is isolated. The
cross section is found to be 2.01±0.30(stat)±0.16(syst) fb.
The corresponding standard model predicted cross section
calculated at next-to-leading order in perturbative quantum
chromodynamics and at leading order in the electroweak
coupling constant is 1.50±0.06 fb. The observed
significance of the WZγ signal is 6.3σ, compared with an
expected significance of 5.0σ.},
Doi = {10.1103/physrevlett.132.021802},
Key = {fds375334}
}
@article{fds375987,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Observation of Wγγ triboson production in proton-proton
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {848},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138400},
Abstract = {This letter reports the observation of W(ℓν)γγ
production in proton-proton collisions. This measurement
uses the full Run 2 sample of events recorded at a
center-of-mass energy of s=13 TeV by the ATLAS detector at
the LHC, corresponding to an integrated luminosity of 140
fb−1. Events with a leptonically-decaying W boson and at
least two photons are considered. The background-only
hypothesis is rejected with an observed and expected
significance of 5.6 standard deviations. The inclusive
fiducial production cross section of W(eν)γγ and
W(μν)γγ events is measured to be σfid=13.8±1.1(stat)+2.1−2.0(syst)±0.1(lumi)
fb, in agreement with the Standard Model
prediction.},
Doi = {10.1016/j.physletb.2023.138400},
Key = {fds375987}
}
@article{fds346193,
Author = {Sangwan, BR and Kotwal, A and Verma, AK},
Title = {Occupational Exposure to Blood and Body Fluids amongst
Health Care Workers in a Teaching Hospital of the Armed
Forces.},
Journal = {Medical journal, Armed Forces India},
Volume = {67},
Number = {1},
Pages = {21-24},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1016/s0377-1237(11)80006-7},
Abstract = {<h4>Background</h4>Health care workers (HCWs) are at risk of
infection with blood-borne viruses in the course of their
work. Over 90% of these infections are occurring in
low-income countries and most are preventable. However, the
situation in the Armed Forces hospitals has always been
thought to be much better than the public health facilities
in India. The focus of the study was on assessing the
exposure frequency amongst HCWs in a teaching hospital in
the Armed Forces.<h4>Methods</h4>A cross-sectional survey
amongst HCWs involved in collecting blood samples and
administering injections in all wards of the hospital was
conducted. Selection of study participants was by simple
random sampling. A pre-tested questionnaire was administered
by unlinked, anonymous method.<h4>Result</h4>Total sample
studied was 70. The proportion of HCWs experiencing exposure
to blood body fluid splash (BBF) and needlestick injury
(NSI) during last one week was 47.1 % and 31.43 %,
respectively. The incidence density of BBF exposure was
537.14 per 100 person years and that of NSI episodes was
228.57 per 100 person years. The reasons for not using
personal protective equipment (PPE) ranged from busy
schedule (37.14%), non use of PPE by co-workers (67.14%),
emergencies (91.43%) risk that patients may get offended by
PPE use by HCWs (27.14%) to discomfort while using PPE
(24.29%). All components of PPE were available as per only
34.29 percent.<h4>Conclusion</h4>The high level of
occupational exposure to blood and body fluids and
consequent risk of infection amongst a group of HCWs in the
Armed Forces highlights the urgent need for interventions to
enhance the occupational safety of workers.},
Doi = {10.1016/s0377-1237(11)80006-7},
Key = {fds346193}
}
@article{fds316846,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Operation and performance of the ATLAS semiconductor
tracker},
Journal = {Journal of Instrumentation},
Volume = {9},
Number = {8},
Pages = {P08009-P08009},
Publisher = {IOP Publishing},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/9/08/P08009},
Abstract = {The semiconductor tracker is a silicon microstrip detector
forming part of the inner tracking system of the ATLAS
experiment at the LHC. The operation and performance of the
semiconductor tracker during the first years of LHC running
are described. More than 99% of the detector modules were
operational during this period, with an average intrinsic
hit efficiency of (99.74±0.04)%. The evolution of the noise
occupancy is discussed, and measurements of the Lorentz
angle, d-ray production and energy loss presented. The
alignment of the detector is found to be stable at the
few-micron level over long periods of time. Radiation damage
measurements, which include the evolution of detector
leakage currents, are found to be consistent with
predictions and are used in the verification of radiation
background simulations.},
Doi = {10.1088/1748-0221/9/08/P08009},
Key = {fds316846}
}
@article{fds362042,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Verzini,
MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C},
Title = {Operation and performance of the ATLAS semiconductor tracker
in LHC Run 2},
Journal = {Journal of Instrumentation},
Volume = {17},
Number = {1},
Year = {2022},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/17/01/P01013},
Abstract = {The semiconductor tracker (SCT) is one of the tracking
systems for charged particles in the ATLAS detector. It
consists of 4088 silicon strip sensor modules. During Run 2
(2015-2018) the Large Hadron Collider delivered an
integrated luminosity of 156 fb−1 to the ATLAS experiment
at a centre-of-mass proton-proton collision energy of 13
TeV. The instantaneous luminosity and pile-up conditions
were far in excess of those assumed in the original design
of the SCT detector. Due to improvements to the data
acquisition system, the SCT operated stably throughout Run
2. It was available for 99.9% of the integrated luminosity
and achieved a data-quality efficiency of 99.85%. Detailed
studies have been made of the leakage current in SCT modules
and the evolution of the full depletion voltage, which are
used to study the impact of radiation damage to the
modules.},
Doi = {10.1088/1748-0221/17/01/P01013},
Key = {fds362042}
}
@article{fds347483,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey,
AJ and Baines, JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura,
AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot,
C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Brown, H and Bruckman de
Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler,
JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Argos, FC and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS},
Title = {Operation and performance of the ATLAS Tile Calorimeter in
Run 1.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {12},
Pages = {987},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6374-z},
Abstract = {The Tile Calorimeter is the hadron calorimeter covering the
central region of the ATLAS experiment at the Large Hadron
Collider. Approximately 10,000 photomultipliers collect
light from scintillating tiles acting as the active material
sandwiched between slabs of steel absorber. This paper gives
an overview of the calorimeter's performance during the
years 2008-2012 using cosmic-ray muon events and
proton-proton collision data at centre-of-mass energies of 7
and 8 TeV with a total integrated luminosity of nearly
30 fb - 1 . The signal reconstruction methods, calibration
systems as well as the detector operation status are
presented. The energy and time calibration methods performed
excellently, resulting in good stability of the calorimeter
response under varying conditions during the LHC Run 1.
Finally, the Tile Calorimeter response to isolated muons and
hadrons as well as to jets from proton-proton collisions is
presented. The results demonstrate excellent performance in
accord with specifications mentioned in the Technical Design
Report.},
Doi = {10.1140/epjc/s10052-018-6374-z},
Key = {fds347483}
}
@article{fds356048,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Optimisation of large-radius jet reconstruction for the
ATLAS detector in 13 TeV proton–proton
collisions},
Journal = {European Physical Journal C},
Volume = {81},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09054-3},
Abstract = {Jet substructure has provided new opportunities for searches
and measurements at the LHC, and has seen continuous
development since the optimization of the large-radius jet
definition used by ATLAS was performed during Run 1. A range
of new inputs to jet reconstruction, pile-up mitigation
techniques and jet grooming algorithms motivate an
optimisation of large-radius jet reconstruction for ATLAS.
In this paper, this optimisation procedure is presented, and
the performance of a wide range of large-radius jet
definitions is compared. The relative performance of these
jet definitions is assessed using metrics such as their
pileup stability, ability to identify hadronically decaying
W bosons and top quarks with large transverse momenta. A new
type of jet input object, called a ‘unified flow object’
is introduced which combines calorimeter- and
inner-detector-based signals in order to achieve optimal
performance across a wide kinematic range. Large-radius jet
definitions are identified which significantly improve on
the current ATLAS baseline definition, and their modelling
is studied using pp collisions recorded by the ATLAS
detector at s=13TeV during 2017.},
Doi = {10.1140/epjc/s10052-021-09054-3},
Key = {fds356048}
}
@article{fds346174,
Author = {Mahesh, SH and Kushwaha, AS and Kotwal, A},
Title = {Pandemic influenza: Experience in a flu OPD of a tertiary
care hospital.},
Journal = {Medical journal, Armed Forces India},
Volume = {70},
Number = {1},
Pages = {39-42},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.06.018},
Abstract = {<h4>Background</h4>In April 2009, Mexican health authorities
announced an outbreak of a novel H1N1 influenza virus, which
subsequently caused a pandemic. The world is now moving into
the post-pandemic period. The experience gained in handling
this pandemic at various levels under different settings has
provided us many lessons for the future.<h4>Objective</h4>To
study the profile of various activities undertaken at flu
screening centre as a response to pandemic influenza in a
tertiary care hospital.<h4>Methods</h4>Record-based study
conducted in a tertiary care hospital of Pune. Required data
was collected from records of flu OPD, ward and local health
authority and interviewing related staff. Study included
data from October 2009 to October 2010.<h4>Results</h4>A
total of 8020 people presenting with influenza like illness
(ILI) were screened in the flu OPD under study. Out of
these, only 388 (4.84%) met clinical criteria where throat
samples were collected, out of which only 81 were found to
be positive (20.88%). Total three fatalities (3.7%)
occurred out of 81 who had tested positive. Most cases of
flu were managed at home (76.54%) while only 19 (23.4%) lab
confirmed cases of H1N1 required hospitalisation.<h4>Conclusion</h4>Majority
of cases of H1N1 (2009) were managed at home. Early
diagnosis, quick initiation of treatment, infection control
measures, and good care at the hospital can effectively
reduce morbidity and mortality in H1N1 pandemic.},
Doi = {10.1016/j.mjafi.2012.06.018},
Key = {fds346174}
}
@article{fds347496,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Dos
Santos, SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann,
D and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E},
Title = {Performance of algorithms that reconstruct missing
transverse momentum in [Formula: see text]= 8 TeV
proton-proton collisions in the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {4},
Pages = {241},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4780-2},
Abstract = {The reconstruction and calibration algorithms used to
calculate missing transverse momentum ([Formula: see text] )
with the ATLAS detector exploit energy deposits in the
calorimeter and tracks reconstructed in the inner detector
as well as the muon spectrometer. Various strategies are
used to suppress effects arising from additional
proton-proton interactions, called pileup, concurrent with
the hard-scatter processes. Tracking information is used to
distinguish contributions from the pileup interactions using
their vertex separation along the beam axis. The performance
of the [Formula: see text] reconstruction algorithms,
especially with respect to the amount of pileup, is
evaluated using data collected in proton-proton collisions
at a centre-of-mass energy of 8 [Formula: see text] during
2012, and results are shown for a data sample corresponding
to an integrated luminosity of [Formula: see text]. The
simulation and modelling of [Formula: see text] in events
containing a <i>Z</i> boson decaying to two charged leptons
(electrons or muons) or a <i>W</i> boson decaying to a
charged lepton and a neutrino are compared to data. The
acceptance for different event topologies, with and without
high transverse momentum neutrinos, is shown for a range of
threshold criteria for [Formula: see text] , and estimates
of the systematic uncertainties in the [Formula: see text]
measurements are presented.},
Doi = {10.1140/epjc/s10052-017-4780-2},
Key = {fds347496}
}
@article{fds315920,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Performance of b-jet identification in the ATLAS
experiment},
Journal = {Journal of Instrumentation},
Volume = {11},
Number = {4},
Pages = {P04008-P04008},
Publisher = {IOP Publishing},
Year = {2016},
Month = {April},
url = {http://dx.doi.org/10.1088/1748-0221/11/04/P04008},
Abstract = {The identification of jets containing b hadrons is important
for the physics programme of the ATLAS experiment at the
Large Hadron Collider. Several algorithms to identify jets
containing b hadrons are described, ranging from those based
on the reconstruction of an inclusive secondary vertex or
the presence of tracks with large impact parameters to
combined tagging algorithms making use of multi-variate
discriminants. An independent b-tagging algorithm based on
the reconstruction of muons inside jets as well as the
b-tagging algorithm used in the online trigger are also
presented. The b-jet tagging efficiency, the c-jet tagging
efficiency and the mistag rate for light flavour jets in
data have been measured with a number of complementary
methods. The calibration results are presented as scale
factors defined as the ratio of the efficiency (or mistag
rate) in data to that in simulation. In the case of b jets,
where more than one calibration method exists, the results
from the various analyses have been combined taking into
account the statistical correlation as well as the
correlation of the sources of systematic
uncertainty.},
Doi = {10.1088/1748-0221/11/04/P04008},
Key = {fds315920}
}
@article{fds356551,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Araque, JP and Ferraz, VA and Pereira,
RA},
Title = {Performance of electron and photon triggers in ATLAS during
LHC Run 2},
Journal = {European Physical Journal C},
Volume = {80},
Number = {1},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7500-2},
Abstract = {Electron and photon triggers covering transverse energies
from 5 GeV to several TeV are essential for the ATLAS
experiment to record signals for a wide variety of physics:
from Standard Model processes to searches for new phenomena
in both proton–proton and heavy-ion collisions. To cope
with a fourfold increase of peak LHC luminosity from 2015 to
2018 (Run 2), to 2.1×1034cm-2s-1, and a similar increase in
the number of interactions per beam-crossing to about 60,
trigger algorithms and selections were optimised to control
the rates while retaining a high efficiency for physics
analyses. For proton–proton collisions, the
single-electron trigger efficiency relative to a
single-electron offline selection is at least 75% for an
offline electron of 31 GeV, and rises to 96% at 60 GeV;
the trigger efficiency of a 25 GeV leg of the primary
diphoton trigger relative to a tight offline photon
selection is more than 96% for an offline photon of 30 GeV.
For heavy-ion collisions, the primary electron and photon
trigger efficiencies relative to the corresponding standard
offline selections are at least 84% and 95%, respectively,
at 5 GeV above the corresponding trigger
threshold.},
Doi = {10.1140/epjc/s10052-019-7500-2},
Key = {fds356551}
}
@article{fds307576,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Performance of jet substructure techniques for large-R jets
in proton-proton collisions at √s=7 TeV using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {9},
Publisher = {Springer Nature},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2013)076},
Abstract = {This paper presents the application of a variety of
techniques to study jet substructure. The performance of
various modified jet algorithms, or jet grooming techniques,
for several jet types and event topologies is investigated
for jets with transverse momentum larger than 300 GeV.
Properties of jets subjected to the mass-drop filtering,
trimming, and pruning algorithms are found to have a reduced
sensitivity to multiple proton-proton interactions, are more
stable at high luminosity and improve the physics potential
of searches for heavy boosted objects. Studies of the
expected discrimination power of jet mass and jet
substructure observables in searches for new physics are
also presented. Event samples enriched in boosted W and Z
bosons and top-quark pairs are used to study both the
individual jet invariant mass scales and the efficacy of
algorithms to tag boosted hadronic objects. The analyses
presented use the full 2011 ATLAS dataset, corresponding to
an integrated luminosity of 4.7 ± 0.1 fb-1 from
proton-proton collisions produced by the Large Hadron
Collider at a centre-of-mass energy of √s=7 TeV. [Figure
not available: see fulltext.] © 2013 Cern for the benefit
of the ATLAS collaboration.},
Doi = {10.1007/JHEP09(2013)076},
Key = {fds307576}
}
@article{fds307717,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, J and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D},
Title = {Performance of missing transverse momentum reconstruction in
proton-proton collisions at√s = 7 TeV with
atlas},
Journal = {European Physical Journal C},
Volume = {72},
Number = {1},
Pages = {1-35},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1844-6},
Abstract = {The measurement of missing transverse momentum in the ATLAS
detector, described in this paper, makes use of the full
event reconstruction and a calibration based on
reconstructed physics objects. The performance of the
missing transverse momentum reconstruction is evaluated
using data collected in pp collisions at a centre-of-mass
energy of 7 TeV in 2010. Minimum bias events and events with
jets of hadrons are used from data samples corresponding to
an integrated luminosity of about 0.3 nb1 and 600 nb1
respectively, together with events containing a Z boson
decaying to two leptons (electrons or muons) or aW boson
decaying to a lepton (electron or muon) and a neutrino, from
a data sample corresponding to an integrated luminosity of
about 36 pb1. An estimate of the systematic uncertainty on
the missing transverse momentum scale is presented. © CERN
for the benefit of the ATLAS collaboration
2011.},
Doi = {10.1140/epjc/s10052-011-1844-6},
Key = {fds307717}
}
@article{fds347482,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini,
D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks,
T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina,
E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioară, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Colasurdo,
L},
Title = {Performance of missing transverse momentum reconstruction
with the ATLAS detector using proton-proton collisions at s
= 13 TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {11},
Pages = {903},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6288-9},
Abstract = {The performance of the missing transverse momentum ( E T
miss ) reconstruction with the ATLAS detector is evaluated
using data collected in proton-proton collisions at the LHC
at a centre-of-mass energy of 13 TeV in 2015. To
reconstruct E T miss , fully calibrated electrons, muons,
photons, hadronically decaying τ -leptons , and jets
reconstructed from calorimeter energy deposits and
charged-particle tracks are used. These are combined with
the soft hadronic activity measured by reconstructed
charged-particle tracks not associated with the hard
objects. Possible double counting of contributions from
reconstructed charged-particle tracks from the inner
detector, energy deposits in the calorimeter, and
reconstructed muons from the muon spectrometer is avoided by
applying a signal ambiguity resolution procedure which
rejects already used signals when combining the various E T
miss contributions. The individual terms as well as the
overall reconstructed E T miss are evaluated with various
performance metrics for scale (linearity), resolution, and
sensitivity to the data-taking conditions. The method
developed to determine the systematic uncertainties of the E
T miss scale and resolution is discussed. Results are shown
based on the full 2015 data sample corresponding to an
integrated luminosity of 3.2 fb - 1 .},
Doi = {10.1140/epjc/s10052-018-6288-9},
Key = {fds347482}
}
@article{fds321076,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa,
M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton,
AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates,
RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer,
F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin,
PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker,
M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall,
A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella,
G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Brown, J and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret,
MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini,
I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo,
F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and El Moursli and RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G},
Title = {Performance of pile-up mitigation techniques for jets in
[Formula: see text] collisions at [Formula: see text] TeV
using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {11},
Pages = {581},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4395-z},
Abstract = {The large rate of multiple simultaneous proton-proton
interactions, or pile-up, generated by the Large Hadron
Collider in Run 1 required the development of many new
techniques to mitigate the adverse effects of these
conditions. This paper describes the methods employed in the
ATLAS experiment to correct for the impact of pile-up on jet
energy and jet shapes, and for the presence of spurious
additional jets, with a primary focus on the large
20.3 [Formula: see text] data sample collected at a
centre-of-mass energy of [Formula: see text]. The energy
correction techniques that incorporate sophisticated
estimates of the average pile-up energy density and tracking
information are presented. Jet-to-vertex association
techniques are discussed and projections of performance for
the future are considered. Lastly, the extension of these
techniques to mitigate the effect of pile-up on jet shapes
using subtraction and grooming procedures is
presented.},
Doi = {10.1140/epjc/s10052-016-4395-z},
Key = {fds321076}
}
@article{fds361307,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei,
D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
ATH and Arguin, JF and Argyropoulos, S},
Title = {Performance of the ATLAS Level-1 topological trigger in
Run 2},
Journal = {European Physical Journal C},
Volume = {82},
Number = {1},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09807-0},
Abstract = {During LHC Run 2 (2015–2018) the ATLAS Level-1
topological trigger allowed efficient data-taking by the
ATLAS experiment at luminosities up to 2.1× 1034 cm- 2s-
1, which exceeds the design value by a factor of two. The
system was installed in 2016 and operated in 2017 and 2018.
It uses Field Programmable Gate Array processors to select
interesting events by placing kinematic and angular
requirements on electromagnetic clusters, jets, τ-leptons,
muons and the missing transverse energy. It allowed to
significantly improve the background event rejection and
signal event acceptance, in particular for Higgs and
B-physics processes.},
Doi = {10.1140/epjc/s10052-021-09807-0},
Key = {fds361307}
}
@article{fds310315,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal,
M},
Title = {Performance of the ATLAS muon trigger in pp collisions at
[Formula: see text] TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {3},
Pages = {120},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3325-9},
Abstract = {The performance of the ATLAS muon trigger system is
evaluated with proton-proton collision data collected in
2012 at the Large Hadron Collider at a centre-of-mass energy
of 8 TeV. It is primarily evaluated using events containing
a pair of muons from the decay of [Formula: see text]
bosons. The efficiency of the single-muon trigger is
measured for muons with transverse momentum [Formula: see
text] GeV, with a statistical uncertainty of less than
0.01 % and a systematic uncertainty of 0.6 %. The
[Formula: see text] range for efficiency determination is
extended by using muons from decays of [Formula: see text]
mesons, [Formula: see text] bosons, and top quarks. The muon
trigger shows highly uniform and stable performance. The
performance is compared to the prediction of a detailed
simulation.},
Doi = {10.1140/epjc/s10052-015-3325-9},
Key = {fds310315}
}
@article{fds354098,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Ferraz, VA and Pereira,
RA},
Title = {Performance of the ATLAS muon triggers in Run
2},
Journal = {Journal of Instrumentation},
Volume = {15},
Number = {9},
Year = {2020},
Month = {September},
url = {http://dx.doi.org/10.1088/1748-0221/15/09/P09015},
Abstract = {The performance of the ATLAS muon trigger system is
evaluated with proton-proton (pp) and heavy-ion (HI)
collision data collected in Run 2 during 2015-2018 at the
Large Hadron Collider. It is primarily evaluated using
events containing a pair of muons from the decay of Z bosons
to cover the intermediate momentum range between 26 GeV and
100 GeV. Overall, the efficiency of the single-muon triggers
is about 68% in the barrel region and 85% in the endcap
region. The pT range for efficiency determination is
extended by using muons from decays of Jψ mesons, W bosons,
and top quarks. The performance in HI collision data is
measured and shows good agreement with the results obtained
in pp collisions. The muon trigger shows uniform and stable
performance in good agreement with the prediction of a
detailed simulation. Dedicated multi-muon triggers with
kinematic selections provide the backbone to beauty,
quarkonia, and low-mass physics studies. The design,
evolution and performance of these triggers are discussed in
detail.},
Doi = {10.1088/1748-0221/15/09/P09015},
Key = {fds354098}
}
@article{fds358687,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA},
Title = {Performance of the ATLAS RPC detector and Level-1 muon
barrel trigger at √s = 13 TeV},
Journal = {Journal of Instrumentation},
Volume = {16},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1088/1748-0221/16/07/P07029},
Abstract = {The ATLAS experiment at the Large Hadron Collider (LHC)
employs a trigger system consisting of a first-level
hardware trigger (L1) and a software-based high-level
trigger. The L1 muon trigger system selects muon candidates,
assigns them to the correct LHC bunch crossing and
classifies them into one of six transverse-momentum
threshold classes. The L1 muon trigger system uses
resistive-plate chambers (RPCs) to generate the muon-induced
trigger signals in the central (barrel) region of the ATLAS
detector. The ATLAS RPCs are arranged in six concentric
layers and operate in a toroidal magnetic field with a
bending power of 1.5 to 5.5 Tm. The RPC detector consists of
about 3700 gas volumes with a total surface area of more
than 4000 m2. This paper reports on the performance of the
RPC detector and L1 muon barrel trigger using 60.8 fb-1 of
proton-proton collision data recorded by the ATLAS
experiment in 2018 at a centre-of-mass energy of 13 TeV.
Detector and trigger performance are studied using Z boson
decays into a muon pair. Measurements of the RPC detector
response, efficiency, and time resolution are reported.
Measurements of the L1 muon barrel trigger efficiencies and
rates are presented, along with measurements of the
properties of the selected sample of muon candidates.
Measurements of the RPC currents, counting rates and mean
avalanche charge are performed using zero-bias collisions.
Finally, RPC detector response and efficiency are studied at
different high voltage and front-end discriminator threshold
settings in order to extrapolate detector response to the
higher luminosity expected for the High Luminosity
LHC.},
Doi = {10.1088/1748-0221/16/07/P07029},
Key = {fds358687}
}
@article{fds347511,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Performance of the ATLAS track reconstruction algorithms in
dense environments in LHC Run 2.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {10},
Pages = {673},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5225-7},
Abstract = {With the increase in energy of the Large Hadron Collider to
a centre-of-mass energy of 13 [Formula: see text] for Run
2, events with dense environments, such as in the cores of
high-energy jets, became a focus for new physics searches as
well as measurements of the Standard Model. These
environments are characterized by charged-particle
separations of the order of the tracking detectors sensor
granularity. Basic track quantities are compared between
3.2 fb[Formula: see text] of data collected by the ATLAS
experiment and simulation of proton-proton collisions
producing high-transverse-momentum jets at a centre-of-mass
energy of 13 [Formula: see text]. The impact of
charged-particle separations and multiplicities on the track
reconstruction performance is discussed. The track
reconstruction efficiency in the cores of jets with
transverse momenta between 200 and 1600 [Formula: see text]
is quantified using a novel, data-driven, method. The method
uses the energy loss, [Formula: see text], to identify pixel
clusters originating from two charged particles. Of the
charged particles creating these clusters, the measured
fraction that fail to be reconstructed is [Formula: see
text] and [Formula: see text] for jet transverse momenta of
200-400 [Formula: see text] and 1400-1600 [Formula: see
text], respectively.},
Doi = {10.1140/epjc/s10052-017-5225-7},
Key = {fds347511}
}
@article{fds356751,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adersberger,
M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Verzini, MJA and Aleksa,
M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos,
SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Armitage, LJ},
Title = {Performance of the ATLAS Transition Radiation Tracker in Run
1 of the LHC: Tracker properties},
Journal = {Journal of Instrumentation},
Volume = {12},
Number = {5},
Year = {2017},
Month = {May},
url = {http://dx.doi.org/10.1088/1748-0221/12/05/P05002},
Abstract = {The tracking performance parameters of the ATLAS Transition
Radiation Tracker (TRT) as part of the ATLAS inner detector
are described in this paper for different data-taking
conditions in proton-proton, proton-lead and lead-lead
collisions at the Large Hadron Collider (LHC). The
performance is studied using data collected during the first
period of LHC operation (Run 1) and is compared with Monte
Carlo simulations. The performance of the TRT, operating
with two different gas mixtures (xenon-based and
argon-based) and its dependence on the TRT occupancy is
presented. These studies show that the tracking performance
of the TRT is similar for the two gas mixtures and that a
significant contribution to the particle momentum resolution
is made by the TRT up to high particle densities.},
Doi = {10.1088/1748-0221/12/05/P05002},
Key = {fds356751}
}
@article{fds307718,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Performance of the ATLAS trigger system in
2010},
Journal = {European Physical Journal C},
Volume = {72},
Number = {1},
Pages = {1-61},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1849-1},
Abstract = {Proton-proton collisions at √S = 7 TeV and heavy ion
collisions at √SNN = 2.76 TeV were produced by the LHC and
recorded using the ATLAS experiment's trigger system in
2010. The LHC is designed with a maximum bunch crossing rate
of 40 MHz and the ATLAS trigger system is designed to record
approximately 200 of these per second. The trigger system
selects events by rapidly identifying signatures of muon,
electron, photon, tau lepton, jet, and B meson candidates,
as well as using global event signatures, such as missing
transverse energy. An overview of the ATLAS trigger system,
the evolution of the system during 2010 and the performance
of the trigger system components and selections based on the
2010 collision data are shown. A brief outline of plans for
the trigger system in 2011 is presented.},
Doi = {10.1140/epjc/s10052-011-1849-1},
Key = {fds307718}
}
@article{fds347501,
Author = {Atlas Collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten,
K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke,
S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda,
E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez
Barajas, CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR},
Title = {Performance of the ATLAS trigger system in
2015.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {5},
Pages = {317},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4852-3},
Abstract = {During 2015 the ATLAS experiment recorded [Formula: see
text] of proton-proton collision data at a centre-of-mass
energy of [Formula: see text]. The ATLAS trigger system is a
crucial component of the experiment, responsible for
selecting events of interest at a recording rate of
approximately 1 kHz from up to 40 MHz of collisions. This
paper presents a short overview of the changes to the
trigger and data acquisition systems during the first long
shutdown of the LHC and shows the performance of the trigger
system and its components based on the 2015 proton-proton
collision data.},
Doi = {10.1140/epjc/s10052-017-4852-3},
Key = {fds347501}
}
@article{fds352491,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Performance of the missing transverse momentum triggers for
the ATLAS detector during Run-2 data taking},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {8},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2020)080},
Abstract = {The factor of four increase in the LHC luminosity, from 0.5
× 1034 cm−2s−1 to 2.0 × 1034cm−2s−1, and the
corresponding increase in pile-up collisions during the
2015–2018 data-taking period, presented a challenge for
the ATLAS trigger, particularly for those algorithms that
select events with missing transverse momentum. The output
data rate at fixed threshold typically increases
exponentially with the number of pile-up collisions, so the
legacy algorithms from previous LHC data-taking periods had
to be tuned and new approaches developed to maintain the
high trigger efficiency achieved in earlier operations. A
study of the trigger performance and comparisons with
simulations show that these changes resulted in event
selection efficiencies of > 98% for this period, meeting and
in some cases exceeding the performance of similar triggers
in earlier run periods, while at the same time keeping the
necessary bandwidth within acceptable limits. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP08(2020)080},
Key = {fds352491}
}
@article{fds375850,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Cardoso, MA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler,
A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Tame, ZPA and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán, SC and Cadamuro,
L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace,
N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini,
G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and El Moursli and RC and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A},
Title = {Performance of the reconstruction of large impact parameter
tracks in the inner detector of ATLAS},
Journal = {The European Physical Journal C},
Volume = {83},
Number = {11},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-12024-6},
Abstract = {<jats:title>Abstract</jats:title><jats:p>Searches for
long-lived particles (LLPs) are among the most promising
avenues for discovering physics beyond the Standard Model at
the Large Hadron Collider (LHC). However, displaced
signatures are notoriously difficult to identify due to
their ability to evade standard object reconstruction
strategies. In particular, the ATLAS track reconstruction
applies strict pointing requirements which limit sensitivity
to charged particles originating far from the primary
interaction point. To recover efficiency for LLPs decaying
within the tracking detector volume, the ATLAS Collaboration
employs a dedicated large-radius tracking (LRT) pass with
loosened pointing requirements. During Run 2 of the LHC, the
LRT implementation produced many incorrectly reconstructed
tracks and was therefore only deployed in small subsets of
events. In preparation for LHC Run 3, ATLAS has
significantly improved both standard and large-radius track
reconstruction performance, allowing for LRT to run in all
events. This development greatly expands the potential
phase-space of LLP searches and streamlines LLP analysis
workflows. This paper will highlight the above achievement
and report on the readiness of the ATLAS detector for
track-based LLP searches in Run 3.</jats:p>},
Doi = {10.1140/epjc/s10052-023-12024-6},
Key = {fds375850}
}
@article{fds354096,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Performance of the upgraded PreProcessor of the ATLAS
Level-1 Calorimeter Trigger},
Journal = {Journal of Instrumentation},
Volume = {15},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1088/1748-0221/15/11/P11016},
Abstract = {The PreProcessor of the ATLAS Level-1 Calorimeter Trigger
prepares the analogue trigger signals sent from the ATLAS
calorimeters by digitising, synchronising, and calibrating
them to reconstruct transverse energy deposits, which are
then used in further processing to identify event features.
During the first long shutdown of the LHC from 2013 to 2014,
the central components of the PreProcessor, the Multichip
Modules, were replaced by upgraded versions that feature
modern ADC and FPGA technology to ensure optimal performance
in the high pile-up environment of LHC Run 2. This paper
describes the features of the new Multichip Modules along
with the improvements to the signal processing
achieved.},
Doi = {10.1088/1748-0221/15/11/P11016},
Key = {fds354096}
}
@article{fds356600,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos, SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Aperio Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz, V and Araujo Pereira, R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Performance of top-quark and W -boson tagging with ATLAS in
Run 2 of the LHC},
Journal = {European Physical Journal C},
Volume = {79},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6847-8},
Abstract = {The performance of identification algorithms (“taggers”)
for hadronically decaying top quarks and W bosons in pp
collisions at s = 13 TeV recorded by the ATLAS experiment
at the Large Hadron Collider is presented. A set of
techniques based on jet shape observables are studied to
determine a set of optimal cut-based taggers for use in
physics analyses. The studies are extended to assess the
utility of combinations of substructure observables as a
multivariate tagger using boosted decision trees or deep
neural networks in comparison with taggers based on
two-variable combinations. In addition, for highly boosted
top-quark tagging, a deep neural network based on jet
constituent inputs as well as a re-optimisation of the
shower deconstruction technique is presented. The
performance of these taggers is studied in data collected
during 2015 and 2016 corresponding to 36.1 fb - 1 for the
tt¯ and γ+ jet and 36.7 fb - 1 for the dijet event
topologies.},
Doi = {10.1140/epjc/s10052-019-6847-8},
Key = {fds356600}
}
@article{fds361714,
Author = {Golling, T and Hance, M and Harris, P and Mangano, ML and McCullough, M and Moortgat, F and Schwaller, P and Torre, R and Agrawal, P and Alves, DSM and Antusch, S and Arbey, A and Auerbach, B and Bambhaniya, G and Battaglia,
M and Bauer, M and Dev, PSB and Boveia, A and Bramante, J and Buchmueller,
O and Buschmann, M and Chakrabortty, J and Chala, M and Chekanov, S and Chen, C-Y and Cheng, H-C and Cirelli, M and Citron, M and Cohen, T and Craig, N and Curtin, D and D'Agnolo, RT and Doglioni, C and Dror, JA and Pree, TD and Dylewsky, D and Ellis, J and Ellis, SAR and Essig, R and Fan,
JJ and Farina, M and Feng, JL and Fox, PJ and Galloway, J and Giudice, G and Gluza, J and Gori, S and Guha, S and Hahn, K and Han, T and Helsens, C and Henriques, A and Iwamoto, S and Jelinski, T and Jung, S and Kahlhoefer,
F and Khoze, VV and Kim, D and Kopp, J and Kotwal, A and Kraemer, M and Lindert, JM and Liu, J and Lou, HK and Love, J and Low, M and Machado, PAN and Mahmoudi, F and Marrouche, J and Martin, A and Mohan, K and Mohapatra,
RN and Nardini, G and Olive, KA and Ostdiek, B and Panico, G and Plehn, T and Proudfoot, J and Qian, Z and Reece, M and Rizzo, T and Roskas, C and Ruderman, J and Ruiz, R and Sala, F and Salvioni, E and Saraswat, P and Schell, T and Schmidt-Hoberg, K and Serra, J and Shadmi, Y and Shelton,
J and Solans, C and Spannowsky, M and Srivastava, T and Stolarski, D and Szafron, R and Taoso, M and Tarem, S and Thalapillil, A and Thamm, A and Tsai, Y and Verhaaren, C and Vignaroli, N and Walsh, JR and Wang, LT and Weiland, C and Wells, J and Williams, C and Wulzer, A and Xue, W and Yu, F and Zheng, B and Zheng, J},
Title = {Physics at a 100 TeV pp collider: beyond the Standard Model
phenomena},
Year = {2016},
Month = {June},
Abstract = {This report summarises the physics opportunities in the
search and study of physics beyond the Standard Model at a
100 TeV pp collider.},
Key = {fds361714}
}
@article{fds212567,
Author = {A.V. Kotwal and ATLAS Collaboration},
Title = {Physics at a High-Luminosity LHC with ATLAS},
Journal = {ATL-PHYS-PUB-2012-004},
Year = {2012},
Month = {October},
Key = {fds212567}
}
@article{fds362581,
Author = {Baur, U and Brock, R and Parsons, J and Albrow, M and Denisov, D and Han,
T and Kotwal, A and Olness, F and Qian, J and Belyaev,
S},
Title = {Physics at Future Hadron Colliders},
Journal = {eConf C},
Volume = {010630},
Pages = {E4001},
Year = {2002},
Month = {January},
Abstract = {We discuss the physics opportunities and detector challenges
at future hadron colliders. As guidelines for energies and
luminosities we use the proposed luminosity and/or energy
upgrade of the LHC (SLHC), and the Fermilab design of a Very
Large Hadron Collider (VLHC). We illustrate the physics
capabilities of future hadron colliders for a variety of new
physics scenarios (supersymmetry, strong electroweak
symmetry breaking, new gauge bosons, compositeness and extra
dimensions). We also investigate the prospects of doing
precision Higgs physics studies at such a machine, and list
selected Standard Model physics rates.},
Key = {fds362581}
}
@article{fds352598,
Author = {Chekanov, SV and Kotwal, AV and Yeh, CH and Yu, SS},
Title = {Physics potential of timing layers in future collider
detectors},
Journal = {Journal of Instrumentation},
Volume = {15},
Number = {9},
Year = {2020},
Month = {September},
url = {http://dx.doi.org/10.1088/1748-0221/15/09/P09021},
Abstract = {The physics potential of timing layers with a few tens of
pico-second resolution in the calorimeters of future
collider detectors is explored. These studies show how such
layers can be used for particle identification and
illustrate the potential for detecting new event signatures
originating from physics beyond the standard
model.},
Doi = {10.1088/1748-0221/15/09/P09021},
Key = {fds352598}
}
@article{fds308254,
Author = {Laymon, CM and Amos, W and Burlein, MG and Fortune, HT and Ekenberg, T and Kotwal, A and O'Donnell, JM and Silk, JD and Zumbro, JD and Morris, CL and Seestrom, SJ and Dhuga, KS and Garnett, R and Rawool-Sullivan, MW and Moore, CF and Morris, SL and Watson, DL},
Title = {Pion elastic and inelastic 21+ scattering on 58,60,62,64Ni
at T pi =180 MeV.},
Journal = {Physical review. C, Nuclear physics},
Volume = {53},
Number = {3},
Pages = {1167-1172},
Year = {1996},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevc.53.1167},
Abstract = {Angular distributions for π+ and π- elastic and inelastic
scattering from the Z=28 closed-proton-shell nuclei
58,50,62,64Ni have been measured at an incident pion kinetic
energy of 180 MeV. Values for the neutron and proton matrix
elements for the transition to the Jπ=2+1 state have been
extracted using the distorted wave impulse approximation in
which the π+ and π- data were fitted simultaneously and
the neutron and proton vibrational transition strengths were
treated as free parameters. While all transitions are
predominantly collective, extracted values of M n|Mp
indicate increasing collectivity as a function of neutron
number and are consistent with the collective limit of N|Z
for 64Ni.},
Doi = {10.1103/physrevc.53.1167},
Key = {fds308254}
}
@article{fds308259,
Author = {Burlein, M and Fortune, HT and Amos, WM and Ekenberg, TL and Kotwal, A and Kutt, PH and O'Donnell, JM and Silk, JD and Boyer, B and Fuentes, A and Johnson, K and Moore, CF and Yoo, SH and Mordechai, S and Morris, CL and Zumbro, JD and Watson, DL and Dhuga, KS},
Title = {Pion inelastic scattering to low-lying positive-parity
states in 20Ne.},
Journal = {Physical review. C, Nuclear physics},
Volume = {51},
Number = {1},
Pages = {88-97},
Year = {1995},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevc.51.88},
Abstract = {We have measured pion inelastic scattering from Ne20 with
180 MeV π+ and π- at 12°and from 15°to 90°in 5°steps
and with 120 MeV π+ from 15°to 90°in 5°steps. We report
here on states in the first four Kπ=0+ bands, including the
6.73MeV 0+ and the 8.78-MeV 6+ levels. Coupled-channels
processes are shown to be important for many states. © 1995
The American Physical Society.},
Doi = {10.1103/physrevc.51.88},
Key = {fds308259}
}
@article{fds308261,
Author = {Burlein, M and Fortune, HT and Amos, WM and Ekenberg, TL and Kotwal, A and Kutt, PH and O'Donnell, JM and Silk, JD and Boyer, B and Fuentes, A and Johnson, K and Moore, CF and Yoo, SH and Mordechai, S and Morris, CL and Zumbro, JD and Watson, DL and Dhuga, KS},
Title = {Pion inelastic scattering to the low-lying broad 2+ in
20Ne.},
Journal = {Physical review. C, Nuclear physics},
Volume = {40},
Number = {2},
Pages = {785-789},
Year = {1989},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevc.40.785},
Abstract = {We have observed the broad 2+ member of the K=04+ band of
Ne20 with the Ne20() reaction at T=120 and 180 MeV and with
Ne20() at T=180 MeV. We find an excitation energy of
9.000.18 MeV and a width of 0.8 MeV. The B(E2) is determined
to be approximately 25 to 35 e2fm4. © 1989 The American
Physical Society.},
Doi = {10.1103/physrevc.40.785},
Key = {fds308261}
}
@article{fds308260,
Author = {Watson, DL and Gilman, R and Morris, CL and Zumbro, JD and Mordechai, S and Burlein, M and Odonnell, JM and Fortune, HT and Kotwal, A and Puttz, J and Silk, JD and McDonald, JS and Moore, CF and Williams, AL and Yoo,
SY},
Title = {Pion-induced double charge exchange on C12, Mg24, S32, and
Ca40},
Journal = {Physical Review C},
Volume = {43},
Number = {3},
Pages = {1318-1320},
Publisher = {American Physical Society (APS)},
Year = {1991},
url = {http://dx.doi.org/10.1103/PhysRevC.43.1318},
Abstract = {Angular distributions for pion-induced double-charge-exchange
(DCX) reaction have been measured at 164 MeV on the T=0
target nuclei C12, Mg24, S32, and Ca40. The data are
compared to calculations using the nucleon interaction model
with realistic wave functions and NN and NN form factors
deduced from fits to previously published DCX data on O16.
The calculations reproduce the general shape of the angular
distributions and the absolute magnitude of the cross
sections to within a factor of two. © 1991 The American
Physical Society.},
Doi = {10.1103/PhysRevC.43.1318},
Key = {fds308260}
}
@article{fds362573,
Author = {Brock, R and Peskin, ME and Agashe, K and Artuso, M and Campbell, J and Dawson, S and Erbacher, R and Gerber, C and Gershtein, Y and Gritsan, A and Hatakeyama, K and Huston, J and Kotwal, A and Logan, H and Luty, M and Melnikov, K and Narain, M and Papucci, M and Petriello, F and Prell, S and Qian, J and Schwienhorst, R and Tully, C and Kooten, RV and Wackeroth,
D and Wang, L and Whiteson, D},
Title = {Planning the Future of U.S. Particle Physics (Snowmass
2013): Chapter 3: Energy Frontier},
Year = {2014},
Month = {January},
Abstract = {These reports present the results of the 2013 Community
Summer Study of the APS Division of Particles and Fields
("Snowmass 2013") on the future program of particle physics
in the U.S. Chapter 3, on the Energy Frontier, discusses the
program of research with high-energy colliders. This area
includes experiments on the Higgs boson, the electroweak and
strong interactions, and the top quark. It also encompasses
direct searches for new particles and interactions at high
energy.},
Key = {fds362573}
}
@article{fds344669,
Author = {Abulencia, A and Adelman, J and Affolder, T and Akimoto, T and Albrow,
MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Behari,
S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carillo, S and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Almenar, CC and Cuevas,
J and Culbertson, R and Cully, JC and Daronco, S and Datta, M and D'Auria,
S and Davies, T and Dagenhart, D and Barbaro, PD and Cecco, SD and Deisher,
A and Lentdecker, GD and Lorenzo, GD and Dell'Orso, M and Paoli, FD and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Dionisi, C and Ruzza, BD and Dittmann, JR and D'Onofrio, M and Dörr, C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg,
C and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, SC and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Lytken, E and MacK, P and MacQueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle,
T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy,
L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard,
PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
I and Sidoti, A},
Title = {Polarizations of J/ψ and ψ(2S) mesons produced in pp̄
collisions at s=1.96TeV},
Journal = {Physical Review Letters},
Volume = {99},
Number = {13},
Pages = {132001},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevLett.99.132001},
Abstract = {We have measured the polarizations of J/ψ and ψ(2S) mesons
as functions of their transverse momentum pT when they are
produced promptly in the rapidity range |y|<0.6 with pT
5GeV/c. The analysis is performed using a data sample with
an integrated luminosity of about 800pb-1 collected by the
CDF II detector. For both vector mesons, we find that the
polarizations become increasingly longitudinal as pT
increases from 5 to 30GeV/c. These results are compared to
the predictions of nonrelativistic quantum chromodynamics
and other contemporary models. The effective polarizations
of J/ψ and ψ(2S) mesons from B-hadron decays are also
reported. © 2007 The American Physical Society.},
Doi = {10.1103/PhysRevLett.99.132001},
Key = {fds344669}
}
@article{fds308049,
Author = {Abulencia, and A, and others},
Title = {Precise measurement of the top quark mass in the lepton+jets
topology at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {18},
Pages = {182002},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.182002},
Abstract = {We present a measurement of the mass of the top quark from
proton-antiproton collisions recorded at the CDF experiment
in Run II of the Fermilab Tevatron. We analyze events from
the single lepton plus jets final state (t[overline
t]-->W+bW-[overline b]-->lnubq[overline q][prime][overline
b]). The top-quark mass is extracted using a direct
calculation of the probability density that each event
corresponds to the t[overline t] final state. The
probability is a function of both the mass of the top quark
and the energy scale of the calorimeter jets, which is
constrained in situ by the hadronic W boson mass. Using 167
events observed in 955 pb-1 of integrated luminosity, we
achieve the single most precise measurement of the top-quark
mass, 170.8$\pm$2.2(stat.)$\pm$1.4(syst.)
GeV/c2.},
Doi = {10.1103/physrevlett.99.182002},
Key = {fds308049}
}
@article{fds307541,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Guimaraes Da Costa and J and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
M and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith,
D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A},
Title = {Precise measurement of the W -boson mass with the Collider
Detector at Fermilab},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072003},
Abstract = {We present a measurement of the W-boson mass, MW, using data
corresponding to 2.2fb-1 of integrated luminosity collected
in pp̄ collisions at s=1.96TeV with the CDF II detector at
the Fermilab Tevatron. The selected sample of 470126 W→eν
candidates and 624708 W→μν candidates yields the
measurement MW=80387±12(stat)±15(syst)=80387±19MeV/c2.
This is the most precise single measurement of the W-boson
mass to date. © 2014 American Physical Society.},
Doi = {10.1103/PhysRevD.89.072003},
Key = {fds307541}
}
@article{fds307709,
Author = {Kotwal, AV and Collaboration, CDF},
Title = {Precise Measurement of the W-Boson Mass with the CDF II
Detector},
Journal = {Phys. Rev. Lett.},
Volume = {108},
Number = {15},
Pages = {151803},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.108.151803},
Abstract = {We have measured the W-boson mass M(W) using data
corresponding to 2.2 fb(-1) of integrated luminosity
collected in pp collisions at sqrt[s] = 1.96 TeV with
the CDF II detector at the Fermilab Tevatron collider.
Samples consisting of 470,126 W → eν candidates and
624,708 W → μν candidates yield the measurement M(W) =
80,387 ± 12(stat.) ± 15(syst.) = 80,387 ± 19 MeV/c2.
This is the most precise measurement of the W-boson mass to
date and significantly exceeds the precision of all previous
measurements combined.},
Doi = {10.1103/physrevlett.108.151803},
Key = {fds307709}
}
@article{fds347503,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho,
J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan,
SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C},
Title = {Precision measurement and interpretation of inclusive W+ ,
W- and Z/γ∗ production cross sections with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {6},
Pages = {367},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4911-9},
Abstract = {High-precision measurements by the ATLAS Collaboration are
presented of inclusive W+→ℓ+ν , W-→ℓ-ν¯ and
Z/γ∗→ℓℓ ( ℓ=e,μ ) Drell-Yan production cross
sections at the LHC. The data were collected in
proton-proton collisions at s=7TeV with an integrated
luminosity of 4.6fb-1 . Differential W+ and W- cross
sections are measured in a lepton pseudorapidity range
|ηℓ|<2.5 . Differential Z/γ∗ cross sections are
measured as a function of the absolute dilepton rapidity,
for |yℓℓ|<3.6 , for three intervals of dilepton mass,
mℓℓ , extending from 46 to 150GeV . The integrated and
differential electron- and muon-channel cross sections are
combined and compared to theoretical predictions using
recent sets of parton distribution functions. The data,
together with the final inclusive e±p scattering
cross-section data from H1 and ZEUS, are interpreted in a
next-to-next-to-leading-order QCD analysis, and a new set of
parton distribution functions, ATLAS-epWZ16, is obtained.
The ratio of strange-to-light sea-quark densities in the
proton is determined more accurately than in previous
determinations based on collider data only, and is
established to be close to unity in the sensitivity range of
the data. A new measurement of the CKM matrix element |Vcs|
is also provided.},
Doi = {10.1140/epjc/s10052-017-4911-9},
Key = {fds347503}
}
@article{fds307939,
Author = {Aaltonen, T and others},
Title = {Precision Measurement of the Ξ(3872) Mass in J/ψ π
+ π- Decays},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {15},
Pages = {152001},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.152001},
Abstract = {We present an analysis of the mass of the X(3872)
reconstructed via its decay to J/ψπ+π- using
2.4 fb-1 of integrated luminosity from pp̅ collisions
at sqrt[s]=1.96 TeV, collected with the CDF II detector
at the Fermilab Tevatron. The possible existence of two
nearby mass states is investigated. Within the limits of our
experimental resolution the data are consistent with a
single state, and having no evidence for two states we set
upper limits on the mass difference between two hypothetical
states for different assumed ratios of contributions to the
observed peak. For equal contributions, the 95% confidence
level upper limit on the mass difference is 3.6 MeV/c2.
Under the single-state model the X(3872) mass is measured to
be 3871.61 ± 0.16(stat) ± 0.19(syst) MeV/c2,
which is the most precise determination to
date.},
Doi = {10.1103/physrevlett.103.152001},
Key = {fds307939}
}
@article{fds308072,
Author = {Abulencia, and A, and others},
Title = {Precision measurement of the top quark mass from dilepton
events at CDF II},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {3},
Pages = {031105},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.031105},
Abstract = {We report a measurement of the top-quark mass, Mt, in the
dilepton decay channel of t[overline t]-->b[script-l][prime]+nu[script-l][prime][overline
b][script-l]-[overline nu ][script-l] using an integrated
luminosity of 1.0 fb-1 of p[overline p] collisions collected
with the CDF II detector. We apply a method that convolutes
a leading-order matrix element with detector resolution
functions to form event-by-event likelihoods; we have
enhanced the leading-order description to describe the
effects of initial-state radiation. The joint likelihood is
the product of the likelihoods from 78 candidate events in
this sample, which yields a measurement of
Mt=164.5$\pm$3.9(stat.)$\pm$3.9(syst.) GeV/c2, the most
precise measurement of Mt in the dilepton
channel.},
Doi = {10.1103/PhysRevD.75.031105},
Key = {fds308072}
}
@article{fds140618,
Author = {Ashutosh V. Kotwal and A. Abulencia et al. [CDF
Collaboration]},
Title = {Precision measurement of the top-quark mass from dilepton
events at CDF II},
Journal = {Physical Review D (Rapid Communication)},
Volume = {75},
Number = {031105},
Year = {2007},
Month = {February},
url = {http://link.aps.org/abstract/PRD/v75/e031105},
Keywords = {top • mass},
Abstract = {We report a measurement of the top-quark mass, Mt, in the
dilepton decay channel of t tbar-->b l nu + b l nu using an
integrated luminosity of 1.0/fb of p-pbar collisions
collected with the CDF II detector. We apply a method that
convolutes a leading-order matrix element with detector
resolution functions to form event-by-event likelihoods; we
have enhanced the leading-order description to describe the
effects of initial-state radiation. The joint likelihood is
the product of the likelihoods from 78 candidate events in
this sample, which yields a measurement of Mt = 164.5 +-
3.9(stat.) +- 3.9(syst.) GeV/c^2, the most precise
measurement of Mt in the dilepton channel.},
Key = {fds140618}
}
@article{fds308104,
Author = {Abulencia, and A, and others},
Title = {Precision top quark mass measurement in the lepton + jets
topology in p anti-p collisions at $\sqrt{s}=$
1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {2},
Pages = {022004},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.022004},
Abstract = {We report two measurements of the top quark mass M_top using
the CDF II detector at the Fermilab Tevatron in a 318 pb-1
data sample observed in the lepton + jets final state. One
method uses an event-based likelihood technique resulting in
M_top = 173.2+2.6_-2.4 (stat.) +/- 3.2 (syst.) GeV/c2 or
173.2+4.1_-40 GeV/c2. The second method reconstructs a top
quark mass in each event using the measured invariant mass
of the hadronically decaying W boson to constrain the jet
energy scale to obtain a value for M_top of 173.5+3.7_-3.6
(stat.) +/- 1.3 (syst.) GeV/c2 or 173.5+3.9_-3.8 GeV/c2. We
take the latter, which is more precise, as our
result.},
Doi = {10.1103/physrevlett.96.022004},
Key = {fds308104}
}
@article{fds307682,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Precision top-quark mass measurement at CDF.},
Journal = {Physical review letters},
Volume = {109},
Number = {15},
Pages = {152003},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.109.152003},
Abstract = {We present a precision measurement of the top-quark mass
using the full sample of Tevatron √s = 1.96 TeV
proton-antiproton collisions collected by the CDF II
detector, corresponding to an integrated luminosity of 8.7
fb(-1). Using a sample of tt¯ candidate events decaying
into the lepton+jets channel, we obtain distributions of the
top-quark masses and the invariant mass of two jets from the
W boson decays from data. We then compare these
distributions to templates derived from signal and
background samples to extract the top-quark mass and the
energy scale of the calorimeter jets with in situ
calibration. The likelihood fit of the templates from signal
and background events to the data yields the single
most-precise measurement of the top-quark mass,
M(top)=172.85±0.71(stat)±0.85(syst) GeV/c(2).},
Doi = {10.1103/physrevlett.109.152003},
Key = {fds307682}
}
@article{fds346205,
Author = {Tendulkar, RD and Chellman-Jeffers, M and Rybicki, LA and Rim, A and Kotwal, A and Macklis, R and Obi, BB},
Title = {Preoperative breast magnetic resonance imaging in early
breast cancer: implications for partial breast
irradiation.},
Journal = {Cancer},
Volume = {115},
Number = {8},
Pages = {1621-1630},
Year = {2009},
Month = {April},
url = {http://dx.doi.org/10.1002/cncr.24172},
Abstract = {<h4>Background</h4>Accelerated partial breast irradiation
(APBI) of patients with early breast cancer is being
investigated on a multi-institutional protocol National
Surgical Adjuvant Breast and Bowel Project (NSABP) B-39/RTOG
0413. Breast magnetic resonance imaging (MRI) is more
sensitive than mammography (MG) and may aid in selection of
patients appropriate for PBI.<h4>Methods</h4>Patients with
newly diagnosed breast cancer or ductal carcinoma in situ
(DCIS) routinely undergo contrast-enhanced, bilateral breast
MRI at the Cleveland Clinic. We retrospectively reviewed the
medical records of all early-stage breast cancer patients
who had a breast MRI, MG, and surgical pathology data at our
institution between June of 2005 and December of 2006. Any
suspicious lesions identified on MRI were further evaluated
by targeted ultrasound +/- biopsy.<h4>Results</h4>A total of
260 patients met eligibility criteria for NSABP B-39/RTOG
0413 by MG, physical exam, and surgical pathology. The
median age was 57 years. DCIS was present in 63 patients,
and invasive breast cancer was found in 197 patients. MRI
identified suspicious lesions in 35 ipsilateral breasts
(13%) and in 16 contralateral breasts (6%). Mammographically
occult, synchronous ipsilateral foci were found by MRI in 11
patients (4.2%), and in the contralateral breast in 4
patients (1.5%). By univariate analysis, lobular histology
(infiltrating lobular carcinoma [ILC]), pathologic T2, and
American Joint Committee on Cancer stage II were
significantly associated with additional ipsilateral
disease. Of patients with ILC histology, 18% had ipsilateral
secondary cancers or DCIS, compared with 3% in the remainder
of histologic subtypes (P = .004). No patient older than 70
years had synchronous cancers or DCIS detected by
MRI.<h4>Conclusions</h4>Breast MRI identified synchronous
mammographically occult foci in 5.8% of early breast cancer
patients who would otherwise be candidates for
APBI.},
Doi = {10.1002/cncr.24172},
Key = {fds346205}
}
@article{fds346177,
Author = {Kumar, P and Londhe, SM and Kotwal, A and Mitra, R},
Title = {Prevalence of malocclusion and orthodontic treatment need in
schoolchildren - An epidemiological study.},
Journal = {Medical journal, Armed Forces India},
Volume = {69},
Number = {4},
Pages = {369-374},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.02.003},
Abstract = {<h4>Background</h4>To ascertain the prevalence of
malocclusion and orthodontic treatment need in
schoolchildren dependent on armed forces personnel. To
review the overall oral health using DMFT index and to
evaluate any relation between increased DMFT index to
existing orthodontic problems.<h4>Method</h4>Five schools
were randomly selected among Army/KV/AF schools and a random
sample of 1200 children aged 10-15 years old attending these
schools dependant on armed forces personnel were selected. A
survey form was filled up after the examination of children
by the principal worker and need for orthodontic treatment
was assessed using index for orthodontic treatment need
(IOTN) and overall oral health status by DMFT index and
totaled. Frontal intra oral photograph in centric occlusion
were taken. Dental Health Component (DHC) of IOTN for all
the patients was marked by one set of orthodontists. The
most severe occlusal trait was identified by the examiner
for any particular patient and the patient was then
categorized according to this most severe trait. AC of the
IOTN was assessed by second orthodontist, individual and a
layperson.<h4>Results</h4>It was observed that prevalence of
malocclusion in the sample was 53.7%. 32.8% (239 males & 154
females) of samples are in need of orthodontic treatment.
55.1% of samples shown no caries risk, 38.1% had moderate
caries risk and 6.8% had high caries risk.<h4>Conclusion</h4>Significant
percentage of the samples are in need for orthodontic
treatment. There is significant relation between higher DMFT
index and orthodontic treatment need. It was found that IOTN
is a reliable and user-friendly index, which can be used for
orthodontic surveys.},
Doi = {10.1016/j.mjafi.2012.02.003},
Key = {fds346177}
}
@booklet{Abbott98,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri,
SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson,
JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and di Loreto, G and Draper, P and Ducros, Y and Dudko,
LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein,
D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak,
Y},
Title = {Probing hard color-singlet exchange in pp̄ collisions at
√s = 630 GeV and 1800 GeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {440},
Number = {1-2},
Pages = {189-202},
Publisher = {Elsevier BV},
Year = {1998},
Month = {November},
url = {http://dx.doi.org/10.1016/S0370-2693(98)01238-6},
Abstract = {We present results on dijet production via hard
color-singlet exchange in proton-antiproton collisions at
√s = 630 GeV and 1800 GeV using the DØ detector. The
fraction of dijet events produced via color-singlet exchange
is measured as a function of jet transverse energy,
separation in pseudorapidity between the two highest
transverse energy jets, and proton-antiproton center-of-mass
energy. The results are consistent with a color-singlet
fraction that increases with an increasing fraction of
quark-initiated processes and inconsistent with two-gluon
models for the hard color-singlet. © 1998 Published by
Elsevier Science B.V. All rights reserved.},
Doi = {10.1016/S0370-2693(98)01238-6},
Key = {Abbott98}
}
@article{fds321128,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bacci,
C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard,
CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho
Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Probing lepton flavour violation via neutrinoless [Formula:
see text] decays with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {232},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4041-9},
Abstract = {This article presents the sensitivity of the ATLAS
experiment to the lepton-flavour-violating decays of
[Formula: see text]. A method utilising the production of
[Formula: see text] leptons via [Formula: see text] decays
is used. This method is applied to the sample of
20.3 fb[Formula: see text] of <i>pp</i> collision data at a
centre-of-mass energy of 8 TeV collected by the ATLAS
experiment at the LHC in 2012. No event is observed passing
the selection criteria, and the observed (expected) upper
limit on the [Formula: see text] lepton branching fraction
into three muons, [Formula: see text], is [Formula: see
text] ([Formula: see text]) at 90 % confidence
level.},
Doi = {10.1140/epjc/s10052-016-4041-9},
Key = {fds321128}
}
@article{fds376062,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Probing the CP nature of the top–Higgs Yukawa coupling in
tt¯H and tH events with H→bb¯ decays using the ATLAS
detector at the LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {849},
Year = {2024},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2024.138469},
Abstract = {The CP properties of the coupling between the Higgs boson
and the top quark are investigated using 139 fb−1 of
proton–proton collision data recorded by the ATLAS
experiment at the LHC at a centre-of-mass energy of s=13
TeV. The CP structure of the top quark–Higgs boson Yukawa
coupling is probed in events with a Higgs boson decaying
into a pair of b-quarks and produced in association with
either a pair of top quarks, tt¯H, or a single top quark,
tH. Events containing one or two electrons or muons are used
for the measurement. Multivariate techniques are used to
select regions enriched in tt¯H and tH events, where
dedicated CP-sensitive observables are exploited. In an
extension of the Standard Model (SM) with a CP-odd admixture
in the top–Higgs Yukawa coupling, the mixing angle between
CP-even and CP-odd couplings is measured to be
α=11−73∘∘+52∘, compatible with the SM prediction
corresponding to α=0.},
Doi = {10.1016/j.physletb.2024.138469},
Key = {fds376062}
}
@article{fds347457,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic, M and Bakalis,
C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
IA},
Title = {Probing the Quantum Interference between Singly and Doubly
Resonant Top-Quark Production in pp Collisions at
sqrt[s]=13 TeV with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {121},
Number = {15},
Pages = {152002},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.121.152002},
Abstract = {This Letter presents a normalized differential cross-section
measurement in a fiducial phase-space region where
interference effects between top-quark pair production and
associated production of a single top quark with a W boson
and a b-quark are significant. Events with exactly two
leptons (ee, μμ, or eμ) and two b-tagged jets that
satisfy a multiparticle invariant mass requirement are
selected from 36.1 fb^{-1} of proton-proton collision
data taken at sqrt[s]=13 TeV with the ATLAS detector at
the LHC in 2015 and 2016. The results are compared with
predictions from simulations using various strategies for
the interference. The standard prescriptions for
interference modeling are significantly different from each
other but are within 2σ of the data. State-of-the-art
predictions that naturally incorporate interference effects
provide the best description of the data in the measured
region of phase space most sensitive to these effects. These
results provide an important constraint on interference
models and will guide future model development and
tuning.},
Doi = {10.1103/physrevlett.121.152002},
Key = {fds347457}
}
@article{fds356756,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Probing the W tb vertex structure in t-channel
single-top-quark production and decay in pp collisions at
√s=8 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {4},
Year = {2017},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2017)124},
Abstract = {To probe the W tb vertex structure, top-quark and W -boson
polarisation observables are measured from t-channel
single-top-quark events produced in proton-proton collisions
at a centre-of-mass energy of 8 TeV. The dataset corresponds
to an integrated luminosity of 20.2 fb−1, recorded with
the ATLAS detector at the LHC. Selected events contain one
isolated electron or muon, large missing transverse momentum
and exactly two jets, with one of them identified as likely
to contain a b-hadron. Stringent selection requirements are
applied to discriminate t-channel single-top-quark events
from background. The polarisation observables are extracted
from asymmetries in angular distributions measured with
respect to spin quantisation axes appropriately chosen for
the top quark and the W boson. The asymmetry measurements
are performed at parton level by correcting the observed
angular distributions for detector effects and hadronisation
after subtracting the background contributions. The measured
top-quark and W -boson polarisation values are in agreement
with the Standard Model predictions. Limits on the imaginary
part of the anomalous coupling gR are also set from
model-independent measurements.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP04(2017)124},
Key = {fds356756}
}
@article{fds310119,
Author = {Kotwal, AV and Hays, C},
Title = {Production and decay of spinning black holes at colliders
and tests of black hole dynamics},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {66},
Number = {11},
Pages = {116005},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.66.116005},
Abstract = {We analyze the angular momentum distribution of black holes
produced in high energy collisions in space-times with extra
spatial dimensions. We show that the black hole spin
significantly affects the energy and angular spectra of
Hawking radiation. Our results show the experimental
sensitivity to the angular momentum distribution and provide
tests of black hole production dynamics. © 2002 The
American Physical Society.},
Doi = {10.1103/PhysRevD.66.116005},
Key = {fds310119}
}
@article{fds310397,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Production of KS0, K*(892) and φ0(1020) in minimum bias
events and KS0 and Λ0 in jets in pp̄ collisions at
√s=1.96 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.88.092005},
Abstract = {We report measurements of the inclusive transverse momentum
(pT) distribution of centrally produced KS0, K±(892), and
φ0(1020) mesons up to pT=10 GeV/c in minimum bias events,
and KS0 and Λ0 particles up to pT=20 GeV/c in jets with
transverse energy between 25 and 160 GeV in pp̄ collisions.
The data were taken with the CDF II detector at the Fermilab
Tevatron at √s=1.96 TeV. We find that as pT increases, the
pT slopes of the three mesons (KS0, K±, and φ) are
similar. And using our previous Λ0 results from minimum
bias events, we show that the ratio of Λ0 to KS0 as a
function of pT in minimum bias events becomes similar to the
fairly constant ratio in jets at pT∼5 GeV/c. This suggests
that the particles with pTâ‰35 GeV/c in minimum bias
events are from "soft" jets, and that the pT slope of
particles in jets is insensitive to light quark flavor (u,
d, or s) and to the number of valence quarks. We also find
that for pT≠24 GeV relatively more Λ0 baryons are
produced in minimum bias events than in jets. © 2013
American Physical Society.},
Doi = {10.1103/PhysRevD.88.092005},
Key = {fds310397}
}
@article{fds341955,
Author = {Aaltonen, T and González, BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Cecco,
SD and Lorenzo, GD and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'errico, M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum, W and Keung,
J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse,
M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, Q and Liu, T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Maksimovic, P and Malik, S and Manca, G and Manousakis-Katsikakis,
A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson,
ME and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Griso, SP and Pagliarone,
C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin,
F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa,
K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson,
GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel,
M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, C and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wen, A and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund,
AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka,
J},
Title = {Production of Λ0, Λ ̄0, Ξ ±, and
Ω± hyperons in pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {1},
Year = {2012},
url = {http://dx.doi.org/10.1103/PhysRevD.86.012002},
Abstract = {We report a set of measurements of inclusive invariant p T
differential cross sections of Λ0, Λ ̄0, Ξ ±, and Ω ±
hyperons reconstructed in the central region with
pseudorapidity |η|<1 and p T up to 10GeV/c. Events are
collected with a minimum-bias trigger in pp̄ collisions at
a center-of-mass energy of 1.96 TeV using the CDF II
detector at the Tevatron Collider. As p T increases, the
slopes of the differential cross sections of the three
particles are similar, which could indicate a universality
of the particle production in p T. The invariant
differential cross sections are also presented for different
charged-particle multiplicity intervals. © 2012 American
Physical Society.},
Doi = {10.1103/PhysRevD.86.012002},
Key = {fds341955}
}
@article{fds307990,
Author = {Aaltonen, T and others},
Title = {Production of ψ(2S) mesons in pp̅ collisions at 1.96
TeV},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {3},
Pages = {031103},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.031103},
Abstract = {We have measured the differential cross section for the
inclusive production of ψ(2S) mesons decaying to μ+μ-
that were produced in prompt or B-decay processes from pp̅
collisions at 1.96 TeV. These measurements have been made
using a data set from an integrated luminosity of
1.1 fb-1 collected by the CDF II detector at Fermilab.
For events with transverse momentum pT(ψ(2S))>2 GeV/c
and rapidity |y(ψ(2S))|<0.6 we measure the integrated
inclusive cross section σ(pp̅ →ψ(2S)X)·Br(ψ(2S)→μ+μ-)
to be 3.29 ± 0.04(stat) ± 0.32(syst) nb.},
Doi = {10.1103/PhysRevD.80.031103},
Key = {fds307990}
}
@article{fds372393,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF},
Title = {Production of ϒ(nS) mesons in Pb + Pb and pp collisions at
5.02 TeV},
Journal = {Physical Review C},
Volume = {107},
Number = {5},
Year = {2023},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevC.107.054912},
Abstract = {A measurement of the production of vector bottomonium
states, ϒ(1S), ϒ(2S), and ϒ(3S), in Pb + Pb and pp
collisions at a center-of-mass energy per nucleon pair of
5.02 TeV is presented. The data correspond to integrated
luminosities of 1.38 nb-1 of Pb + Pb data collected in 2018,
0.44 nb-1 of Pb + Pb data collected in 2015, and 0.26 fb-1
of pp data collected in 2017 by the ATLAS detector at the
Large Hadron Collider. The measurements are performed in the
dimuon decay channel for transverse momentum pμμT < 30
GeV, absolute rapidity |yμμ| < 1.5, and Pb + Pb event
centrality 0-80%. The production rates of the three
bottomonium states in Pb + Pb collisions are compared with
those in pp collisions to extract the nuclear modification
factors as functions of event centrality, pμμT, and
|yμμ|. In addition, the suppression of the excited states
relative to the ground state is studied. The results are
compared with theoretical model calculations.},
Doi = {10.1103/PhysRevC.107.054912},
Key = {fds372393}
}
@article{fds347480,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou,
EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot,
C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RMB and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
DL and Bristow, TM and Britton, D and Britzger, D and Brock, I and Brock,
R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F},
Title = {Prompt and non-prompt J / ψ and ψ ( 2 S ) suppression at
high transverse momentum in 5.02 TeV Pb+Pb collisions with
the ATLAS experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {9},
Pages = {762},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6219-9},
Abstract = {A measurement of J / ψ and ψ ( 2 S ) production is
presented. It is based on a data sample from Pb+Pb
collisions at s NN = 5.02 TeV and <i>pp</i> collisions at s
= 5.02 TeV recorded by the ATLAS detector at the LHC in
2015, corresponding to an integrated luminosity of 0.42 nb -
1 and 25 pb - 1 in Pb+Pb and <i>pp</i>, respectively. The
measurements of per-event yields, nuclear modification
factors, and non-prompt fractions are performed in the
dimuon decay channel for 9 < p T μ μ < 40 GeV in dimuon
transverse momentum, and - 2 < y μ μ < 2 in rapidity.
Strong suppression is found in Pb+Pb collisions for both
prompt and non-prompt J / ψ , increasing with event
centrality. The suppression of prompt ψ ( 2 S ) is observed
to be stronger than that of J / ψ , while the suppression
of non-prompt ψ ( 2 S ) is equal to that of the non-prompt
J / ψ within uncertainties, consistent with the expectation
that both arise from <i>b</i>-quarks propagating through the
medium. Despite prompt and non-prompt J / ψ arising from
different mechanisms, the dependence of their nuclear
modification factors on centrality is found to be quite
similar.},
Doi = {10.1140/epjc/s10052-018-6219-9},
Key = {fds347480}
}
@article{fds347479,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
IA},
Title = {Prompt and non-prompt J / ψ elliptic flow in Pb+Pb
collisions at s NN = 5.02 Tev with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {9},
Pages = {784},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6243-9},
Abstract = {The elliptic flow of prompt and non-prompt J / ψ was
measured in the dimuon decay channel in Pb+Pb collisions at
s NN = 5.02 TeV with an integrated luminosity of 0.42 nb
- 1 with the ATLAS detector at the LHC. The prompt and
non-prompt signals are separated using a two-dimensional
simultaneous fit of the invariant mass and pseudo-proper
decay time of the dimuon system from the J / ψ decay. The
measurement is performed in the kinematic range of dimuon
transverse momentum and rapidity 9 < p T < 30 GeV , | y |
< 2 , and 0-60% collision centrality. The elliptic flow
coefficient, v 2 , is evaluated relative to the event plane
and the results are presented as a function of transverse
momentum, rapidity and centrality. It is found that prompt
and non-prompt J / ψ mesons have non-zero elliptic flow.
Prompt J / ψ v 2 decreases as a function of p T , while for
non-prompt J / ψ it is, with limited statistical
significance, consistent with a flat behaviour over the
studied kinematic region. There is no observed dependence on
rapidity or centrality.},
Doi = {10.1140/epjc/s10052-018-6243-9},
Key = {fds347479}
}
@article{fds356621,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos,
S},
Title = {Properties of g →b b at small opening angles in pp
collisions with the ATLAS detector at √s=13
TeV},
Journal = {Physical Review D},
Volume = {99},
Number = {5},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.99.052004},
Abstract = {The fragmentation of high-energy gluons at small opening
angles is largely unconstrained by present measurements.
Gluon splitting to b-quark pairs is a unique probe into the
properties of gluon fragmentation because identified
b-tagged jets provide a proxy for the quark daughters of the
initial gluon. In this study, key differential distributions
related to the g→bb process are measured using 33 fb-1 of
s=13 TeV pp collision data recorded by the ATLAS experiment
at the LHC in 2016. Jets constructed from charged-particle
tracks, clustered with the anti-kt jet algorithm with radius
parameter R=0.2, are used to probe angular scales below the
R=0.4 jet radius. The observables are unfolded to particle
level in order to facilitate direct comparisons with
predictions from present and future simulations. Multiple
significant differences are observed between the data and
parton shower Monte Carlo predictions, providing input to
improve these predictions of the main source of background
events in analyses involving boosted Higgs bosons decaying
into b-quarks.},
Doi = {10.1103/PhysRevD.99.052004},
Key = {fds356621}
}
@article{fds356573,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Properties of jet fragmentation using charged particles
measured with the ATLAS detector in pp collisions at s =13
TeV},
Journal = {Physical Review D},
Volume = {100},
Number = {5},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.100.052011},
Abstract = {This paper presents a measurement of quantities related to
the formation of jets from high-energy quarks and gluons
(fragmentation). Jets with transverse momentum 100 GeV
<pT<2.5 TeV and pseudorapidity |η|<2.1 from an integrated
luminosity of 33 fb-1 of s=13 TeV proton-proton collisions
are reconstructed with the ATLAS detector at the Large
Hadron Collider. Charged-particle tracks with pT>500 MeV and
|η|<2.5 are used to probe the detailed structure of the
jet. The fragmentation properties of the more forward and
the more central of the two leading jets from each event are
studied. The data are unfolded to correct for detector
resolution and acceptance effects. Comparisons with parton
shower Monte Carlo generators indicate that existing models
provide a reasonable description of the data across a wide
range of phase space, but there are also significant
differences. Furthermore, the data are interpreted in the
context of quark- and gluon-initiated jets by exploiting the
rapidity dependence of the jet flavor fraction. A first
measurement of the charged-particle multiplicity using
model-independent jet labels (topic modeling) provides a
promising alternative to traditional quark and gluon
extractions using input from simulation. The simulations
provide a reasonable description of the quark-like data
across the jet pT range presented in -this measurement, but
the gluon-like data have systematically fewer charged
particles than the simulation.},
Doi = {10.1103/PhysRevD.100.052011},
Key = {fds356573}
}
@article{fds307856,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Properties of jets measured from tracks in proton-proton
collisions at center-of-mass energy √s=7TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {84},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2011},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.84.054001},
Doi = {10.1103/PhysRevD.84.054001},
Key = {fds307856}
}
@booklet{Adams96,
Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dietrich, FS and Dougherty, W and Dreyer, T and Eckardt, V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kobrak, HG and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and Novak, J and O'Day, S and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Ramberg, EJ},
Title = {Proton and deuteron structure functions in muon scattering
at 470 GeV.},
Journal = {Physical review. D, Particles and fields},
Volume = {54},
Number = {5},
Pages = {3006-3056},
Year = {1996},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevd.54.3006},
Doi = {10.1103/physrevd.54.3006},
Key = {Adams96}
}
@article{fds307966,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and González,
BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos,
J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa, T and Artikov,
A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI},
Title = {Publisher's Note: Search for hadronic decays of W and Z
bosons in photon events in pp̄ collisions at
s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {80},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.80.079901},
Doi = {10.1103/PhysRevD.80.079901},
Key = {fds307966}
}
@article{fds347512,
Author = {Singhal, S and Bhattachar, SA and Paliwal, V and Malhotra, VK and Addya,
K and Kotwal, A},
Title = {Pulmonary Embolism in Young Natives of High
Altitude.},
Journal = {Heart views : the official journal of the Gulf Heart
Association},
Volume = {17},
Number = {2},
Pages = {62-65},
Year = {2016},
Month = {April},
url = {http://dx.doi.org/10.4103/1995-705x.185115},
Abstract = {Thrombotic events are relatively common in high altitude
areas and known to occur in young soldiers working at high
altitude without usual risk factors associated with
thrombosis at sea-level. However, till now, cases with
thrombotic events were reported only in lowlanders staying
at high altitude. These two cases of pulmonary embolism
demonstrate that thrombotic events can occur in highlanders
after a prolonged stay at the extreme altitude.},
Doi = {10.4103/1995-705x.185115},
Key = {fds347512}
}
@article{fds308179,
Author = {Abbott, B and Abdesselam, A and Abolins, M and Abramov, V and Acharya,
BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Davis, GA and Davis, K and De, K and Del
Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
T and Feher, S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grünendahl, S and Gupta,
A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Illingworth, R and Ito, AS and Jaffré, M and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov,
AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski,
S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov, VE and Landsberg, G and Leflat, A and Leggett, C and Lehner,
F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann,
J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin, MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald, J and McMahon, T and Melanson, HL and Meng,
XC and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea,
D and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Nunnemann, T and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu,
S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan, S and Ramberg,
E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon,
J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev,
V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yip,
K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
EG and Zylberstejn, A},
Title = {Quasi-model-independent search for new high p(T) physics at
D0.},
Journal = {Physical review letters},
Volume = {86},
Number = {17},
Pages = {3712-3717},
Year = {2001},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.86.3712},
Abstract = {We apply a quasi-model-independent strategy ("Sleuth") to
search for new high p(T) physics in approximately 100 pb(-1)
of pp collisions at square root of (s) = 1.8 TeV collected
by the D0 experiment during 1992-1996 at the Fermilab
Tevatron. We systematically analyze many exclusive final
states and demonstrate sensitivity to a variety of models
predicting new phenomena at the electroweak scale. No
evidence of new high p(T) physics is observed.},
Doi = {10.1103/physrevlett.86.3712},
Key = {fds308179}
}
@article{fds308188,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev,
VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett,
JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings,
MAC and Cutts, D and Davis, GA and Davis, K and De, K and Jong, SJ and Del
Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A},
Title = {Quasi-model-independent search for new physics at large
transverse momentum},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {64},
Number = {1},
Pages = {120041-1200424},
Publisher = {American Physical Society (APS)},
Year = {2001},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.64.012004},
Abstract = {We apply a quasi-model-independent strategy (“SLEUTH”)
to search for new high [Formula Presented] physics in ≈100
[Formula Presented] of [Formula Presented] collisions at
[Formula Presented] collected by the DØ experiment during
1992–1996 at the Fermilab Tevatron. Over 32 [Formula
Presented] [Formula Presented] [Formula Presented] and
[Formula Presented] exclusive final states are
systematically analyzed for hints of physics beyond the
standard model. Simultaneous sensitivity to a variety of
models predicting new phenomena at the electroweak scale is
demonstrated by testing the method on a particular signature
in each set of final states. No evidence of new high
[Formula Presented] physics is observed in the course of
this search, and we find that 89% of an ensemble of
hypothetical similar experimental runs would have produced a
final state with a candidate signal more interesting than
the most interesting observed in these data. © 2001 The
American Physical Society.},
Doi = {10.1103/PhysRevD.64.012004},
Key = {fds308188}
}
@article{fds307730,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Rapidity gap cross sections measured with the ATLAS detector
in pp collisions at √s =7 TeV},
Journal = {European Physical Journal C},
Volume = {72},
Number = {3},
Pages = {1-31},
Publisher = {Springer Nature},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-1926-0},
Abstract = {Pseudorapidity gap distributions in proton-proton collisions
at √s = 7 TeV are studied using a minimum bias data sample
with an integrated luminosity of 7.1 μb<sup>−1</sup>.
Cross sections are measured differentially in terms of
Δη<sup>F</sup>, the larger of the pseudorapidity regions
extending to the limits of the ATLAS sensitivity, at η =
±4.9, in which no final state particles are produced above
a transverse momentum threshold p<sup>cut</sup><inf>T</inf>.
The measurements span the region 0 < Δη<sup>F</sup> < 8
for 200 MeV < p<sup>cut</sup><inf>T</inf> < 800 MeV. At
small Δη<sup>F</sup>, the data test the reliability of
hadronisation models in describing rapidity and transverse
momentum fluctuations in final state particle production.
The measurements at larger gap sizes are dominated by
contributions from the single diffractive dissociation
process (pp →Xp), enhanced by double dissociation (pp →
XY) where the invariant mass of the lighter of the two
dissociation systems satisfies M<inf>Y</inf> < 7 GeV. The
resulting cross section is dσ/dΔη<sup>F</sup> ≈1 mb for
Δη<sup>F</sup> > 3. The large rapidity gap data are used
to constrain the value of the Pomeron intercept appropriate
to triple Regge models of soft diffraction. The cross
section integrated over all gap sizes is compared with other
LHC inelastic cross section measurements.},
Doi = {10.1140/epjc/s10052-012-1926-0},
Key = {fds307730}
}
@article{fds346171,
Author = {Patrikar, S and Basannar, DR and Bhatti, VK and Kotwal, A and Gupta, RM and Grewal, RS},
Title = {Rate of decline in CD4 count in HIV patients not on
antiretroviral therapy.},
Journal = {Medical journal, Armed Forces India},
Volume = {70},
Number = {2},
Pages = {134-138},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1016/j.mjafi.2013.08.005},
Abstract = {<h4>Background</h4>The progressive decline in the CD4 count
in HIV patients leads to a more general decline in immune
functioning. The study has been carried out to determine the
decline in CD4 count in HIV patients.<h4>Methods</h4>The
study was conducted in a medical college hospital at
Maharashtra. The information on baseline CD4 count was
gathered from positive patient records registered in the
central disease registry. The baseline CD4 count was the
first count of CD4 obtained when the patient is diagnosed as
HIV positive and further two subsequent readings. The time
from baseline (t1) till the last CD4 count (t2) was divided
into the different quartiles and the median decline in CD4
count in each quartile was determined. As the time between
the two CD4 count measurements was not uniform the rate of
change in CD4 was measured with respect to time as [X
(t2) - X (t1)/(t2 - t1)]. Correlation was assessed using
correlation coefficient.<h4>Results</h4>As the CD4 counts
were following skewed distribution, the normality was
achieved by cuberoot transformation. The overall rate of
decline in CD4 count was estimated to be 35 cells/μL per
year with 95% confidence interval (CI) as (17.01, 85.04).
The correlation coefficient between decline in CD4 and the
initial CD4 count in the four time quartiles was
(r = -0.51; p = 0.001, r = -0.79; p = 0.000,
r = -0.48; p = 0.015 and r = -0.80; p = 0.000)
respectively. The median decline in the CD4 count in 0-6
months was 3 cells/μL, in (6-11) months was approximately
26 cells/μL, in (11-21.5) months was 30 cells/μL and in
more than 21.5 months the median decline was 52
cells/μL.<h4>Conclusions</h4>There was a progressive
decline in the CD4 count following HIV infection. An
understanding of the influence of decline in CD4 count in
HIV patients not on ART is important for clinical management
of HIV disease.},
Doi = {10.1016/j.mjafi.2013.08.005},
Key = {fds346171}
}
@article{fds331391,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and De Jong and SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros,
Y},
Title = {Ratio of isolated photon cross sections in pp¯
Collisions at √s = 630 and 1800 GeV},
Journal = {Physical Review Letters},
Volume = {87},
Number = {25},
Pages = {251805-1-251805-7},
Publisher = {American Physical Society (APS)},
Year = {2001},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.87.251805},
Abstract = {The inclusive cross section for production of isolated
photons has been measured in pp¯ collisions at √s = 630
GeV with the D0 detector at the Fermilab Tevatron Collider.
The photons span a transverse energy (ET) range from 7-49
GeV and have pseudorapidity |η| < 2.5. This measurement is
combined with the previous D0 result at √s = 1800 GeV to
form a ratio of the cross sections. Comparison of
next-to-leading-order QCD with the measured cross section at
630 GeV and the ratio of cross sections show satisfactory
agreement in most of the ET range. © 2001 American Physical
Society.},
Doi = {10.1103/PhysRevLett.87.251805},
Key = {fds331391}
}
@article{fds308191,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Gilmartin, R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grudberg, P and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Ito, AS and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kehoe, R and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov, VE and Landsberg, G and Leflat, A and Lehner,
F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann,
J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Maciel,
AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin,
MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy,
R and McDonald, J and McMahon, T and Melanson, HL and Meng, XC and Merkin,
M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mincer,
A and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan,
LJ and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno,
M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan,
S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sculli, J and Sen, N and Shabalina,
E and Shankar, HC and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink,
M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot,
AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White,
A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood,
DR and Yamada, R and Yamin, P and Yasuda, T and Yip, K and Youssef, S and Yu,
J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zhu, ZH and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
EG and Zylberstejn, A and D0 Collaboration},
Title = {Ratio of jet cross sections at square root of s = 630 GeV
and 1800 GeV.},
Journal = {Physical review letters},
Volume = {86},
Number = {12},
Pages = {2523-2528},
Year = {2001},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.86.2523},
Abstract = {The D0 Collaboration has measured the inclusive jet cross
section in barpp collisions at square root of s = 630 GeV.
The results for pseudorapidities (eta)<0.5 are combined with
our previous results at square root of s = 1800 GeV to form
a ratio of cross sections with smaller uncertainties than
either individual measurement. Next-to-leading-order QCD
predictions show excellent agreement with the measurement at
630 GeV; agreement is also satisfactory for the ratio.
Specifically, despite a 10% to 15% difference in the
absolute magnitude, the dependence of the ratio on jet
transverse momentum is very similar for data and
theory.},
Doi = {10.1103/physrevlett.86.2523},
Key = {fds308191}
}
@article{fds308181,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Gilmartin, R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grudberg, P and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Ito, AS and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kehoe, R and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov, VE and Landsberg, G and Leflat, A and Lehner,
F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann,
J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Maciel,
AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin,
MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy,
R and McDonald, J and McMahon, T and Melanson, HL and Meng, XC and Merkin,
M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mincer,
A and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan,
LJ and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno,
M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan,
S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sculli, J and Sen, N and Shabalina,
E and Shankar, HC and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink,
M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot,
AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White,
A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood,
DR and Yamada, R and Yamin, P and Yasuda, T and Yip, K and Youssef, S and Yu,
J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zhu, ZH and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
EG and Zylberstejn, A},
Title = {Ratios of multijet Cross Sections in p p collisions at
radical(s) = 1.8 TeV.},
Journal = {Physical review letters},
Volume = {86},
Number = {10},
Pages = {1955-1960},
Year = {2001},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.86.1955},
Abstract = {We report on a study of the ratio of inclusive three-jet to
inclusive two-jet production cross sections as a function of
total transverse energy in p&pmacr; collisions at a
center-of-mass energy sqrt[s] = 1.8 TeV, using data
collected with the D0 detector during the 1992-1993 run of
the Fermilab Tevatron Collider. The measurements are used to
deduce preferred renormalization scales in perturbative
O(alpha(3)(s)) QCD calculations in modeling soft-jet
emission.},
Doi = {10.1103/physrevlett.86.1955},
Key = {fds308181}
}
@article{fds354162,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Reconstruction and identification of boosted di-τ systems
in a search for Higgs boson pairs using 13 TeV proton-proton
collision data in ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2020)163},
Abstract = {In this paper, a new technique for reconstructing and
identifying hadronically decaying τ+τ− pairs with a
large Lorentz boost, referred to as the di-τ tagger, is
developed and used for the first time in the ATLAS
experiment at the Large Hadron Collider. A benchmark di-τ
tagging selection is employed in the search for resonant
Higgs boson pair production, where one Higgs boson decays
into a boosted bb¯ pair and the other into a boosted
τ+τ− pair, with two hadronically decaying τ-leptons in
the final state. Using 139 fb−1 of proton-proton collision
data recorded at a centre-of-mass energy of 13 TeV, the
efficiency of the di-τ tagger is determined and the
background with quark- or gluon-initiated jets misidentified
as di-τ objects is estimated. The search for a heavy,
narrow, scalar resonance produced via gluon-gluon fusion and
decaying into two Higgs bosons is carried out in the mass
range 1–3 TeV using the same dataset. No deviations from
the Standard Model predictions are observed, and 95%
confidence-level exclusion limits are set on this model.
[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP11(2020)163},
Key = {fds354162}
}
@article{fds316852,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus,
M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {Reconstruction of hadronic decay products of tau leptons
with the ATLAS experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {295},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4110-0},
Abstract = {This paper presents a new method of reconstructing the
individual charged and neutral hadrons in tau decays with
the ATLAS detector. The reconstructed hadrons are used to
classify the decay mode and to calculate the visible
four-momentum of reconstructed tau candidates, significantly
improving the resolution with respect to the calibration in
the existing tau reconstruction. The performance of the
reconstruction algorithm is optimised and evaluated using
simulation and validated using samples of [Formula: see
text] and [Formula: see text]+jets events selected from
proton-proton collisions at a centre-of-mass energy
[Formula: see text], corresponding to an integrated
luminosity of 5 [Formula: see text].},
Doi = {10.1140/epjc/s10052-016-4110-0},
Key = {fds316852}
}
@article{fds347500,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL},
Title = {Reconstruction of primary vertices at the ATLAS experiment
in Run 1 proton-proton collisions at the
LHC.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {5},
Pages = {332},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4887-5},
Abstract = {This paper presents the method and performance of primary
vertex reconstruction in proton-proton collision data
recorded by the ATLAS experiment during Run 1 of the LHC.
The studies presented focus on data taken during 2012 at a
centre-of-mass energy of [Formula: see text] TeV. The
performance has been measured as a function of the number of
interactions per bunch crossing over a wide range, from one
to seventy. The measurement of the position and size of the
luminous region and its use as a constraint to improve the
primary vertex resolution are discussed. A longitudinal
vertex position resolution of about [Formula: see text] is
achieved for events with high multiplicity of reconstructed
tracks. The transverse position resolution is better than
[Formula: see text] and is dominated by the precision on the
size of the luminous region. An analytical model is proposed
to describe the primary vertex reconstruction efficiency as
a function of the number of interactions per bunch crossing
and of the longitudinal size of the luminous region.
Agreement between the data and the predictions of this model
is better than 3% up to seventy interactions per bunch
crossing.},
Doi = {10.1140/epjc/s10052-017-4887-5},
Key = {fds347500}
}
@article{fds346213,
Author = {Bains, R and Kotwal, A and Saeed, W},
Title = {Recurrent carpal tunnel syndrome in a child due to
fibrolipomatous hamartoma of the median nerve successfully
treated by limited excision and decompression.},
Journal = {Journal of plastic, reconstructive & aesthetic surgery :
JPRAS},
Volume = {59},
Number = {12},
Pages = {1394-1397},
Year = {2006},
Month = {January},
url = {http://dx.doi.org/10.1016/j.bjps.2006.01.016},
Abstract = {We present a case of recurrent carpal tunnel syndrome in a
child caused by fibrolipomatous hamartoma of the median
nerve which was successfully treated by limited excision of
the fibrolipomatous tissue and decompression.},
Doi = {10.1016/j.bjps.2006.01.016},
Key = {fds346213}
}
@article{fds346175,
Author = {Shega, JW and Andrew, M and Kotwal, A and Lau, DT and Herr, K and Ersek, M and Weiner, DK and Chin, MH and Dale, W},
Title = {Relationship between persistent pain and 5-year mortality: a
population-based prospective cohort study.},
Journal = {Journal of the American Geriatrics Society},
Volume = {61},
Number = {12},
Pages = {2135-2141},
Year = {2013},
Month = {December},
url = {http://dx.doi.org/10.1111/jgs.12554},
Abstract = {<h4>Objectives</h4>To assess the association between
self-reported noncancer pain and 5-year mortality.<h4>Design</h4>Cohort.<h4>Setting</h4>Community-dwelling
older adults.<h4>Participants</h4>Canadian Study of Health
and Aging 1996 wave.<h4>Measurements</h4>Registrar of Vital
Statistics-established 5-year mortality. Noncancer pain was
assessed using the 5-point verbal descriptor scale,
dichotomized into no or very mild versus moderate, severe,
or very severe pain. Frailty was the accumulation of health
deficits. Cognitive status (Modified Mini-Mental State
Examination) and depressed mood (five-item mental health
screening questionnaire) were also assessed. Multivariable
logistic regression and Cox proportional hazards were used
to analyze the relationship between pain and 5-year
mortality.<h4>Results</h4>Of 5,703 participants, 4,694
(82.3%) had complete data for analysis; 1,663 of these
(35.4%) reported moderate, severe, or very severe pain, and
1,343 (28.6%) had died at 5-year follow-up. Four hundred
ninety-six of those who died (29.8%) reported moderate,
severe, or very severe pain and 847 (27.9%) no or very mild
pain. Multivariate logistic analysis found that individuals
with moderate, severe, or very severe pain had lower odds of
5-year mortality than those with no or very mild pain (odds
ratio=0.78, 95% confidence interval (CI)=0.66-0.92; P<.001).
The risk of death was lower in persons reporting moderate or
greater pain than in those with no or very mild pain
(HR=0.85, 95% CI=0.75-0.96; P=.01). An interaction between
pain and sex explained this effect. Men with pain were not
significantly more likely than men without pain to die
(HR=1.00, 95% CI=0.84-1.19; P=.99), whereas women without
pain (HR=0.54, 95% CI=0.47-0.63; P<0.01) and women with pain
(HR=0.40; CI=0.33-0.47; P<.01) had less risk of death than
men without and with pain, respectively.<h4>Conclusion</h4>Older
women with pain were less likely to die within 5 years than
older women without pain, men in pain, or men without
pain.},
Doi = {10.1111/jgs.12554},
Key = {fds346175}
}
@article{fds346209,
Author = {Varma, PP and Hooda, AK and Sinha, T and Chopra, GS and Karan, SC and Sethi, GS and Badwal, S and Kotwal, A},
Title = {Renal Transplantation - An Experience of 500
Patients.},
Journal = {Medical journal, Armed Forces India},
Volume = {63},
Number = {2},
Pages = {107-111},
Year = {2007},
Month = {April},
url = {http://dx.doi.org/10.1016/s0377-1237(07)80049-9},
Abstract = {<h4>Background</h4>Renal transplantation is the treatment
modality of choice for patients with end stage kidney
failure. We present our experience of graft and patient
survival of initial 500 renal transplants performed between
May 1991 and July 2006, at Army Hospital (R&R).<h4>Material
and methods</h4>All patients received triple drug
immunosuppression with cyclosporine/tacrolimus,
azathioprine/ mycophenolate mofetil and steroids. Patients
in high risk group received induction therapy with IL-2
receptor blockers/anti-thymocyte globulin.<h4>Results</h4>Majority
of the recipients (79%) were males, whereas majority of the
donors (59.4%) were females. In the donor profile, 385 (77%)
transplants were live related, 108 (21.6 %) were spousal and
7 (1.4%) were cadaveric transplants. Mean age of the donors
and recipients was 42.11 ± 11.53 years (range 19-72 years)
and 33 ± 9.39 years (range 5-60 years) respectively. Eighty
two patients (16.4%) were lost to follow up and the present
data on rejections, patients and graft survival pertains to
418 patients. These patients have been followed up for a
mean period of 2.63 years (SE, 0.122; median 1.8 years;
range 0-13.36 years). Acute rejection episodes occurred in
115 (27.3%) patients and 95% of these could be reversed with
steroids/ATG. Sixty eight patients (16%) have died on
follow-up. Our one-year, 5 year and 10 year estimated graft
survival is 95.4% (SE, 0.01), 80.5% (SE, 0.03) and 53.1%
(SE, 0.09) respectively and patient survival at one year is
93.2% (SE, 0.01). The estimated graft and patient survival
in our series is 9.83 (95% CI, 8.92-10.73) and 9.80
(8.93-10.67) years respectively.<h4>Conclusion</h4>This
centre's short-term graft survival of 95.4% is comparable to
the best centres of the world.},
Doi = {10.1016/s0377-1237(07)80049-9},
Key = {fds346209}
}
@article{fds347515,
Author = {Kotwal, A},
Title = {Reply to: Regarding the Article: Does Iodine Excess Lead to
Hypothyroidism? Evidence from A Case-Control Study in
India.},
Journal = {Archives of medical research},
Volume = {47},
Number = {2},
Pages = {146-147},
Year = {2016},
Month = {February},
url = {http://dx.doi.org/10.1016/j.arcmed.2016.05.003},
Doi = {10.1016/j.arcmed.2016.05.003},
Key = {fds347515}
}
@article{fds356574,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Resolution of the ATLAS muon spectrometer monitored drift
tubes in LHC Run 2},
Journal = {Journal of Instrumentation},
Volume = {14},
Number = {9},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1088/1748-0221/14/09/P09011},
Abstract = {The momentum measurement capability of the ATLAS muon
spectrometer relies fundamentally on the intrinsic
single-hit spatial resolution of the monitored drift tube
precision tracking chambers. Optimal resolution is achieved
with a dedicated calibration program that addresses the
specific operating conditions of the 354 000 high-pressure
drift tubes in the spectrometer. The calibrations consist of
a set of timing offsets and drift time to drift distance
transfer relations, and result in chamber resolution
functions. This paper describes novel algorithms to obtain
precision calibrations from data collected by ATLAS in LHC
Run 2 and from a gas monitoring chamber, deployed in a
dedicated gas facility. The algorithm output consists of a
pair of correction constants per chamber which are applied
to baseline calibrations, and determined to be valid for the
entire ATLAS Run 2. The final single-hit spatial resolution,
averaged over 1172 monitored drift tube chambers, is 81.7 ±
2.2 μm.},
Doi = {10.1088/1748-0221/14/09/P09011},
Key = {fds356574}
}
@article{fds346208,
Author = {Anand, SS and Sood, V and Kumar, PG and Sinha, I and Kotwal,
A},
Title = {Retrospective Analysis of Thyroid Cancer
Patients.},
Journal = {Medical journal, Armed Forces India},
Volume = {64},
Number = {1},
Pages = {7-10},
Year = {2008},
Month = {January},
url = {http://dx.doi.org/10.1016/s0377-1237(08)80136-0},
Abstract = {<h4>Background</h4>Thyroid cancer is a spectrum of neoplasms
and manifests in varied forms. The issues related to
presentation, management and outcome of patients with
thyroid malignancy are highlighted.<h4>Methods</h4>Retrospective
analysis of 70 patients and survival analysis for event free
survival was done.<h4>Result</h4>Papillary carcinomas
constituted 88 percent followed by follicular cancers at
nine percent of all cancers. Females were affected more than
males in the ratio of 2.2: 1. Mean age of presentation for
papillary cancer was 39 years and for follicular 50 years.
Sixteen percent patients had regional and 10 percent distant
metastases. Seventeen percent showed raised serum
thyroglobulin and 29 percent had an abnormal whole body scan
during the follow up. Relapse rate were similar in those
receiving 30 mCi of radioiodine and in those receiving more
than 30 mCi.<h4>Conclusion</h4>The study shows that tumour
marker thyroglobulin has higher negative predictive value.
Overall prognosis for differentiated thyroid cancers is
good.},
Doi = {10.1016/s0377-1237(08)80136-0},
Key = {fds346208}
}
@article{fds310300,
Author = {Bandurin, D and Bernardi, G and Gerber, C and Junk, T and Juste, A and Kotwal, A and Lewis, J and Mesropian, C and Schellman, H and Sekaric, J and Toback, D and Van Kooten and R and Vellidis, C and Zivkovic,
L},
Title = {Review of physics results from the Tevatron},
Journal = {International Journal of Modern Physics A},
Volume = {30},
Number = {6},
Pages = {1541001-1541001},
Publisher = {World Scientific Pub Co Pte Lt},
Year = {2015},
Month = {February},
ISSN = {0217-751X},
url = {http://dx.doi.org/10.1142/S0217751X15410018},
Abstract = {We present a comprehensive review of the physics results
obtained by the CDF and D0 collaborations up to summer 2014,
with emphasis on those achieved in the Run II of the
Tevatron collider which delivered a total integrated
luminosity of 10 fb-1 at $\sqrt{s} = 1.96~{\rm TeV}$. The
results are presented in six main physics topics: QCD, Heavy
Flavor, Electroweak, Top quark, Higgs boson and searches for
New Particles and Interactions. The characteristics of the
accelerator, detectors, and the techniques used to achieve
these results are also briefly summarized.},
Doi = {10.1142/S0217751X15410018},
Key = {fds310300}
}
@article{fds310314,
Author = {Kotwal, AV and Schellman, H and Sekaric, J},
Title = {Review of physics results from the Tevatron: Electroweak
physics},
Journal = {International Journal of Modern Physics A},
Volume = {30},
Number = {6},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1142/S0217751X15410043},
Abstract = {We summarize an extensive Tevatron (1984-2011) electroweak
physics program that involves a variety of W and Z boson
precision measurements. The relevance of these studies using
single and associated gauge boson production to our
understanding of the electroweak sector, quantum
chromodynamics and searches for new physics is emphasized.
We discuss the importance of the W boson mass measurement,
the W/Z boson distributions and asymmetries, and diboson
studies. We highlight the recent Tevatron measurements and
prospects for the final Tevatron measurements.},
Doi = {10.1142/S0217751X15410043},
Key = {fds310314}
}
@article{fds346187,
Author = {Gupta, SK and Kotwal, J and Kotwal, A and Dhall, A and Garg,
S},
Title = {Role of homocysteine & MTHFR C677T gene polymorphism as risk
factors for coronary artery disease in young
Indians.},
Journal = {The Indian journal of medical research},
Volume = {135},
Number = {4},
Pages = {506-512},
Year = {2012},
Month = {April},
Abstract = {<h4>Background & objectives</h4>Hyperhomocysteinaemia (HCA)
either due to mutation of MTHFR gene or deficiency of
vitamin B 12 and folic acid, has been reported as a risk
factor for coronary artery disease (CAD). The present study
was aimed to determine plasma homocysteine (Hcy) levels and
to evaluate MTHFR C677T gene polymorphism as risk factors
for CAD, and to study the role of Hcy in conjunction with a
few other risk factors of CAD in young Indians. The effect
of vitamin B12 and folic acid supplements on the raised
plasma Hcy levels in patients of CAD was also
assessed.<h4>Methods</h4>The present study included 199
consecutive angiography confirmed CAD patients, <45 yr of
age, without any other known pro- coagulant state and 200
age- and sex-matched healthy controls. Fasting blood samples
were collected in EDTA and plasma Hcy was estimated by ELISA
test and the MTHFR C677T polymorphism detection was carried
out by PCR-RFLP method.<h4>Results</h4>Significant
difference (P<0.001) was found between mean fasting levels
of plasma Hcy in cases (22.14 ± 10.62 μmol/l) and controls
(17.38 ± 8.46 μmol/l) with an Odds ratio as 1.93 (95% CI,
1.27-2.94). Levels of cholesterol, LDL, and triglycerides
were significantly (P<0.001) higher in cases compared with
controls.<h4>Interpretation & conclusions</h4>Our study
showed significant correlation between hyperhomocysteinaemia
and coronary artery disease. Multivariate analysis by
logistic regression of the various risk factors of CAD,
found high levels of Hcy, cholesterol, LDL and low levels of
HDL and smoking as independent predictors of CAD when all
other factors were controlled. Significant post-treatment
decrease found in HCA was easily modifiable by vitamin
intervention irrespective to their CT or TT genotype of
C677T MTHFR gene. Further studies to look at the plasma
levels of folate and cobalamines and their association with
Hcy are required to be done.},
Key = {fds346187}
}
@article{fds373611,
Author = {Kotwal, AV and Matias, J and Mauri, A and Tong, T and Varnhorst,
L},
Title = {Round table on Standard Model Anomalies},
Journal = {15th Conference on Quark Confinement and the Hadron
Spectrum, Confinement 2022},
Year = {2022},
Month = {January},
url = {http://dx.doi.org/10.1051/epjconf/202227401006},
Abstract = {This contribution to “The XVth Quark confinement and the
Hadron spectrum conference" covers a description, both
theoretical and experimental, of the present status of a set
of very different anomalies. The discussion ranges from the
long standing b → sℓℓ anomalies, (g − 2) and the new
MW anomaly.},
Doi = {10.1051/epjconf/202227401006},
Key = {fds373611}
}
@article{fds307896,
Author = {Aaltonen, and T, and others},
Title = {Search for $R$-Parity Violating Decays of Sneutrinos to
$e\mu{}$, $\mu{}\tau{}$, and $e\tau{}$ Pairs in $pp[over
\ifmmode\bar\else\textasciimacron\fi{}]$ Collisions at
$\sqrt{s}=1.96\,\,TeV$},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {19},
Pages = {191801},
Publisher = {American Physical Society},
Year = {2010},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.191801},
Abstract = {We present a search for supersymmetric neutrino ν
production using the Tevatron pp collision data collected
with the CDF II detector and corresponding to an integrated
luminosity of 1 fb-1. We focus on the scenarios predicted by
the R-parity violating (RPV) supersymmetric models in which
sneutrinos decay to two charged leptons of different flavor.
With the data consistent with the standard model
expectations, we set upper limits on σ(pp→ν)×BR(ν→eμ,μτ,eτ)
and use these results to constrain the RPV couplings as a
function of the sneutrino mass.},
Doi = {10.1103/PhysRevLett.105.191801},
Key = {fds307896}
}
@article{fds307903,
Author = {Aaltonen, and T, and others},
Title = {Search for $WW$ and $WZ$ resonances decaying to electron,
missing $E_T$, and two jets in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {24},
Pages = {241801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.241801},
Abstract = {http://arxiv.org/abs/1004.4946},
Doi = {10.1103/PhysRevLett.104.241801},
Key = {fds307903}
}
@article{fds308092,
Author = {Abulencia, and A, and others},
Title = {Search for $Z^\prime \to e^+ e^-$ using dielectron mass and
angular distribution},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {21},
Pages = {211801},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.211801},
Abstract = {We report results from a search for Z' bosons in high-mass
dielectron events produced in p anti-p collisions at
s**(1/2) = 1.96 TeV. The data were recorded with the CDF II
detector at the Fermilab Tevatron and correspond to an
integrated luminosity of 0.45 fb-1. To identify the Z' -->
e+ e- signal, both the dielectron invariant mass
distribution and the angular distribution of the electron
pair are used. No evidence for a signal is found, and 95\%
confidence level lower limits are set on the Z' mass for
several models.},
Doi = {10.1103/physrevlett.96.211801},
Key = {fds308092}
}
@article{fds310277,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
Title = {Search for a Charged Higgs Boson Produced in the
Vector-Boson Fusion Mode with Decay H(±)→W(±)Z using pp
Collisions at √s=8 TeV with the ATLAS
Experiment.},
Journal = {Physical review letters},
Volume = {114},
Number = {23},
Pages = {231801},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.114.231801},
Abstract = {A search for a charged Higgs boson, H(±), decaying to a
W(±) boson and a Z boson is presented. The search is based
on 20.3 fb(-1) of proton-proton collision data at a
center-of-mass energy of 8 TeV recorded with the ATLAS
detector at the LHC. The H(±) boson is assumed to be
produced via vector-boson fusion and the decays W(±)→qq'
and Z→e(+)e(-)/μ(+)μ(-) are considered. The search is
performed in a range of charged Higgs boson masses from 200
to 1000 GeV. No evidence for the production of an H(±)
boson is observed. Upper limits of 31-1020 fb at 95% C.L.
are placed on the cross section for vector-boson fusion
production of an H(±) boson times its branching fraction to
W(±)Z. The limits are compared with predictions from the
Georgi-Machacek Higgs triplet model.},
Doi = {10.1103/physrevlett.114.231801},
Key = {fds310277}
}
@article{fds310285,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for a CP-odd Higgs boson decaying to Zh in pp
collisions at √s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {744},
Pages = {163-183},
Publisher = {Elsevier BV},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2015.03.054},
Abstract = {A search for a heavy, CP-odd Higgs boson, A, decaying into a
Z boson and a 125 GeV Higgs boson, h, with the ATLAS
detector at the LHC is presented. The search uses
proton–proton collision data at a centre-of-mass energy of
8 TeV corresponding to an integrated luminosity of 20.3
fb−1. Decays of CP-even h bosons to ττ or bb pairs with
the Z boson decaying to electron or muon pairs are
considered, as well as h→bb decays with the Z boson
decaying to neutrinos. No evidence for the production of an
A boson in these channels is found and the 95% confidence
level upper limits derived for σ(gg→A)×BR(A→Zh)×BR(h→ff¯)
are 0.098–0.013 pb for f=τ and 0.57–0.014 pb for f=b in
a range of mA=220–1000 GeV. The results are combined and
interpreted in the context of two-Higgs-doublet
models.},
Doi = {10.1016/j.physletb.2015.03.054},
Key = {fds310285}
}
@article{fds307704,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Anzá, F and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Fuks, B and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for a dark matter candidate produced in association
with a single top quark in pp collisions at
√[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {20},
Pages = {201802},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.201802},
Abstract = {We report a new search for dark matter in a data sample of
an integrated luminosity of 7.7 fb-1 of Tevatron
pp[over ¯] collisions at √[s]=1.96 TeV, collected by
the CDF II detector. We search for production of a
dark-matter candidate, D, in association with a single top
quark. We consider the hadronic decay mode of the top quark
exclusively, yielding a final state of three jets with
missing transverse energy. The data are consistent with the
standard model; we thus set 95% confidence level upper
limits on the cross section of the process pp[over ¯]→t+D
as a function of the mass of the dark-matter candidate. The
limits are approximately 0.5 pb for a dark-matter particle
with mass in the range of 0-150 GeV/c2.},
Doi = {10.1103/physrevlett.108.201802},
Key = {fds307704}
}
@article{fds307561,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Search for a dijet resonance in events with jets and missing
transverse energy in pp̄ collisions at √s=1.96
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.88.092004},
Abstract = {We report on a search for a dijet resonance in events with
only two or three jets and a large imbalance in the total
event transverse momentum. This search is sensitive to the
possible production of a new particle in association with a
W or Z boson, where the boson decays leptonically with one
or more neutrinos in the final state. We use the full data
set collected by the CDF II detector at the Tevatron
collider at a proton-antiproton center-of-mass energy of
1.96 TeV. These data correspond to an integrated luminosity
of 9.1 fb -1. We study the invariant mass distribution of
the two jets with highest transverse energy. We find good
agreement between data and standard model background
expectations and measure the combined cross section for WW,
WZ, and ZZ production to be 13.8-2.7+3.0 pb. No significant
anomalies are observed in the mass spectrum, and 95%
credibility level upper limits are set on the production
rates of a potential new particle in association with a W or
Z boson. © 2013 American Physical Society.},
Doi = {10.1103/PhysRevD.88.092004},
Key = {fds307561}
}
@article{fds307946,
Author = {Aaltonen, T and others},
Title = {Search for a Fermiophobic Higgs Boson Decaying into
Diphotons in pp̅ Collisions at sqrt[s]=1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {6},
Pages = {061803},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.061803},
Abstract = {A search for a narrow diphoton mass resonance is presented
based on data from 3.0 fb-1 of integrated luminosity
from pp̅ collisions at sqrt[s]=1.96 TeV collected by
the CDF experiment. No evidence of a resonance in the
diphoton mass spectrum is observed, and upper limits are set
on the cross section times branching fraction of the
resonant state as a function of Higgs boson mass. The
resulting limits exclude Higgs bosons with masses below
106 GeV/c2 at a 95% Bayesian credibility level for one
fermiophobic benchmark model.},
Doi = {10.1103/physrevlett.103.061803},
Key = {fds307946}
}
@article{fds307792,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
A},
Title = {Search for a fermiophobic Higgs boson in the diphoton decay
channel with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {9},
Pages = {1-18},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2157-0},
Abstract = {A search for a fermiophobic Higgs boson using diphoton
events produced in proton-proton collisions at a
centre-of-mass energy of √s = 7 TeV is performed using
data corresponding to an integrated luminosity of 4.9
fb−1collected by the ATLAS experiment at the Large Hadron
Collider. A specific benchmark model is considered where all
the fermion couplings to the Higgs boson are set to zero and
the bosonic couplings are kept at the Standard Model values
(fermiophobic Higgs model). The largest excess with respect
to the background-only hypothesis is found at 125.5 GeV,
with a local significance of 2.9 standard deviations, which
reduces to 1.6 standard deviations when taking into account
the look-elsewhere effect. The data exclude the fermiophobic
Higgs model in the ranges 110.0–118.0 GeV and
119.5–121.0 GeV at 95 % confidence level.},
Doi = {10.1140/epjc/s10052-012-2157-0},
Key = {fds307792}
}
@booklet{Abachi97c,
Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Boehnlein, AA and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg,
M and Di Loreto and G and Draper, P and Drinkard, J and Alitti, J and Dudko,
LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga, MK and Featherly,
J and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y},
Title = {Search for a Fourth Generation Charge -1/3 Quark via Flavor
Changing Neutral Current Decay},
Journal = {Physical Review Letters},
Volume = {78},
Number = {20},
Pages = {3818-3823},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.78.3818},
Abstract = {We report on a search for pair production of a fourth
generation charge -1/3 quark (b’) in pp collisions at s =
1.8 TeV by the DØ experiment at the Fermilab Tevatron using
an integrated luminosity of 93 pb-1. Both b’ quarks are
assumed to decay via flavor changing neutral currents
(FCNC). The search uses the signatures γ + 3 jets + μ-tag
and 2γ + 2 jets. We see no significant excess of events
over the expected background. We place an upper limit on the
production cross section times branching fraction that is
well below theoretical expectations for a b’ decaying
exclusively via FCNC for b’ masses up to mz + mb. © 1996
American Physical Society.},
Doi = {10.1103/PhysRevLett.78.3818},
Key = {Abachi97c}
}
@article{fds356572,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Search for a heavy charged boson in events with a charged
lepton and missing transverse momentum from pp collisions at
s =13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {100},
Number = {5},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.100.052013},
Abstract = {A search for a heavy charged-boson resonance decaying into a
charged lepton (electron or muon) and a neutrino is
reported. A data sample of 139 fb-1 of proton-proton
collisions at s=13 TeV collected with the ATLAS detector at
the LHC during 2015-2018 is used in the search. The observed
transverse mass distribution computed from the lepton and
missing transverse momenta is consistent with the
distribution expected from the Standard Model, and upper
limits on the cross section for pp→W′→ℓν are
extracted (ℓ=e or μ). These vary between 1.3 pb and 0.05
fb depending on the resonance mass in the range between 0.15
and 7.0 TeV at 95% confidence level for the electron and
muon channels combined. Gauge bosons with a mass below 6.0
and 5.1 TeV are excluded in the electron and muon channels,
respectively, in a model with a resonance that has couplings
to fermions identical to those of the Standard Model W
boson. Cross-section limits are also provided for resonances
with several fixed Γ/m values in the range between 1% and
15%. Model-independent limits are derived in single-bin
signal regions defined by a varying minimum transverse mass
threshold. The resulting visible cross-section upper limits
range between 4.6 (15) pb and 22 (22) ab as the threshold
increases from 130 (110) GeV to 5.1 (5.1) TeV in the
electron (muon) channel.},
Doi = {10.1103/PhysRevD.100.052013},
Key = {fds356572}
}
@article{fds307858,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoroś, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Search for a heavy gauge boson decaying to a charged lepton
and a neutrino in 1 fb-1 of pp collisions at √s
= 7 TeV using the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {705},
Number = {1-2},
Pages = {28-46},
Publisher = {Elsevier BV},
Year = {2011},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2011.09.093},
Abstract = {The ATLAS detector at the LHC is used to search for
high-mass states, such as heavy charged gauge bosons (W'),
decaying to a charged lepton (electron or muon) and a
neutrino. Results are presented based on the analysis of pp
collisions at a center-of-mass energy of 7 TeV corresponding
to an integrated luminosity of 1.04 fb-1. No excess above
Standard Model expectations is observed. A W' with
Sequential Standard Model couplings is excluded at the 95%
confidence level for masses up to 2.15 TeV.},
Doi = {10.1016/j.physletb.2011.09.093},
Key = {fds307858}
}
@article{fds356362,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for a heavy Higgs boson decaying into a Z boson and
another heavy Higgs boson in the ℓℓbb and ℓℓWW final
states in pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {5},
Year = {2021},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09117-5},
Abstract = {A search for a heavy neutral Higgs boson, A, decaying into a
Z boson and another heavy Higgs boson, H, is performed using
a data sample corresponding to an integrated luminosity of
139 fb- 1 from proton–proton collisions at s=13 TeV
recorded by the ATLAS detector at the LHC. The search
considers the Z boson decaying into electrons or muons and
the H boson into a pair of b-quarks or W bosons. The mass
range considered is 230–800 GeV for the A boson and
130–700 GeV for the H boson. The data are in good
agreement with the background predicted by the Standard
Model, and therefore 95% confidence-level upper limits for
σ×B(A→ZH)×B(H→bborH→WW) are set. The upper limits
are in the range 0.0062–0.380 pb for the H→ bb channel
and in the range 0.023–8.9 pb for the H→ WW channel. An
interpretation of the results in the context of
two-Higgs-doublet models is also given.},
Doi = {10.1140/epjc/s10052-021-09117-5},
Key = {fds356362}
}
@article{fds336449,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Search for a heavy Higgs boson decaying into a Z boson and
another heavy Higgs boson in the ℓℓbb final state in pp
collisions at √s= 13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {783},
Pages = {392-414},
Publisher = {Elsevier BV},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2018.07.006},
Abstract = {A search for a heavy neutral Higgs boson, A, decaying into a
Z boson and another heavy Higgs boson, H, is performed using
a data sample corresponding to an integrated luminosity of
36.1 fb−1 from proton–proton collisions at s=13 TeV
recorded in 2015 and 2016 by the ATLAS detector at the Large
Hadron Collider. The search considers the Z boson decaying
to electrons or muons and the H boson into a pair of
b-quarks. No evidence for the production of an A boson is
found. Considering each production process separately, the
95% confidence-level upper limits on the pp→A→ZH
production cross-section times the branching ratio H→bb
are in the range of 14–830 fb for the gluon–gluon fusion
process and 26–570 fb for the b-associated process for the
mass ranges 130–700 GeV of the H boson and 230–800 GeV
of the A boson. The results are interpreted in the context
of two-Higgs-doublet models.},
Doi = {10.1016/j.physletb.2018.07.006},
Key = {fds336449}
}
@article{fds356787,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for a heavy narrow resonance decaying to eμ eτ or
μτ with the ATLAS detector in √s=7 TeV pp collisions at
the LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {723},
Number = {1-3},
Pages = {15-32},
Year = {2013},
Month = {June},
url = {http://dx.doi.org/10.1016/j.physletb.2013.04.035},
Abstract = {This Letter presents the results of a search for a heavy
particle decaying into an e±μ∓, e±τ∓, or μ±τ∓
final state in pp collisions at s=7 TeV. The data were
recorded with the ATLAS detector at the LHC during 2011 and
correspond to an integrated luminosity of 4.6 fb−1. No
significant excess above the Standard Model expectation is
observed, and exclusions at 95% confidence level are placed
on the cross section times branching ratio for the
production of an R-parity-violating supersymmetric tau
sneutrino. For a sneutrino mass of 500 (2000) GeV, the
observed limits on the production cross section times
branching ratio are 3.2 (1.4) fb, 42 (17) fb, and 40 (18) fb
for the eμ eτ and μτ modes, respectively. These results
considerably extend constraints from Tevatron
experiments.},
Doi = {10.1016/j.physletb.2013.04.035},
Key = {fds356787}
}
@article{fds310407,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, T and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, A and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D},
Title = {Search for a heavy neutral particle decaying into an
electron and a muon using 1 fb-1 of atlas
data},
Journal = {European Physical Journal C},
Volume = {71},
Number = {12},
Publisher = {Springer Nature},
Year = {2011},
Month = {December},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1809-9},
Abstract = {A search is presented for a high mass neutral particle that
decays directly to the e±μ∓ final state. The data sample
was recorded by the ATLAS detector in √ s = 7 TeV pp
collisions at the LHC from March to June 2011 and
corresponds to an integrated luminosity of 1.07 fb-1. The
data are found to be consistent with the Standard Model
background. The high e±μ∓ mass region is used to set 95%
confidence level upper limits on the production of two
possible new physics processes: tau sneutrinos in an
R-parity violating supersymmetric model and Z'-like vector
bosons in a lepton flavor violating model.},
Doi = {10.1140/epjc/s10052-011-1809-9},
Key = {fds310407}
}
@article{fds310272,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C and Conti, G},
Title = {Search for a Heavy Neutral Particle Decaying to eμ, eτ, or
μτ in pp Collisions at sqrt[s]=8 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {3},
Pages = {031801},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.115.031801},
Abstract = {This Letter presents a search for a heavy neutral particle
decaying into an opposite-sign different-flavor dilepton
pair, e^{±}μ^{∓}, e^{±}τ^{∓}, or μ^{±}τ^{∓}
using 20.3 fb^{-1} of pp collision data at
sqrt[s]=8 TeV collected by the ATLAS detector at the
LHC. The numbers of observed candidate events are compatible
with the standard model expectations. Limits are set on the
cross section of new phenomena in two scenarios: the
production of ν[over ˜]_{τ} in R-parity-violating
supersymmetric models and the production of a
lepton-flavor-violating Z^{'} vector boson.},
Doi = {10.1103/physrevlett.115.031801},
Key = {fds310272}
}
@article{fds307702,
Author = {Aaltonen, T and Adelman, J and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo,
KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Rao, K and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for a heavy particle decaying to a top quark and a
light quark in pp ¯ collisions at √s=1.96
TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {21},
Pages = {211805},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.211805},
Abstract = {We present a search for a new heavy particle X produced in
association with a top quark, pp[over ¯]→t(X→t[over
¯]q) or pp[over ¯]→t[over ¯](X[over ¯]→tq[over ¯]),
where q stands for up quarks and down quarks. Such a
particle may explain the recent anomalous measurements of
top-quark forward-backward asymmetry. If the light-flavor
quark (q) is reconstructed as a jet (j), this gives a t[over
¯]+j or t+j resonance in tt[over ¯]+jet events, a
previously unexplored experimental signature. In a sample of
events with exactly one lepton, missing transverse momentum
and at least five jets, corresponding to an integrated
luminosity of 8.7 fb(-1) collected by the CDF II detector,
we find the data to be consistent with the standard model.
We set cross-section upper limits on the production (pp[over
¯]→Xt or X[over ¯]t[over ¯]) at 95% confidence level
from 0.61 pb to 0.02 pb for X masses ranging from 200
GeV/c(2) to 800 GeV/c(2), respectively.},
Doi = {10.1103/physrevlett.108.211805},
Key = {fds307702}
}
@article{fds307748,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
G},
Title = {Search for a heavy Standard Model Higgs boson in the channel
H→ZZ→ℓ+ℓ-qq̄ using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {707},
Number = {1},
Pages = {27-45},
Publisher = {Elsevier BV},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2011.11.056},
Abstract = {A search for a heavy Standard Model Higgs boson decaying via
H→ZZ→ℓ+ℓ-qq̄, where ℓ=e, μ, is presented. The
search is performed using a data set of pp collisions at
√s=7 TeV, corresponding to an integrated luminosity of
1.04 fb-1 collected in 2011 by the ATLAS detector at the
CERN LHC collider. No significant excess of events above the
estimated background is found. Upper limits at 95%
confidence level on the production cross section (relative
to that expected from the Standard Model) of a Higgs boson
with a mass in the range between 200 and 600 GeV are
derived. Within this mass range, there is at present
insufficient sensitivity to exclude a Standard Model Higgs
boson. For a Higgs boson with a mass of 360 GeV, where the
sensitivity is maximal, the observed and expected cross
section upper limits are factors of 1.7 and 2.7,
respectively, larger than the Standard Model prediction. ©
2011 CERN.},
Doi = {10.1016/j.physletb.2011.11.056},
Key = {fds307748}
}
@article{fds320776,
Author = {ATLAS Collaboration},
Title = {Search for a heavy top-quark partner in final states with
two leptons with the ATLAS detector at the
LHC},
Journal = {JHEP},
Volume = {1211},
Number = {11},
Pages = {094},
Publisher = {Springer Nature},
Year = {2012},
url = {http://dx.doi.org/10.1007/JHEP11(2012)094},
Abstract = {http://dx.doi.org/10.1007/JHEP11(2012)094},
Doi = {10.1007/JHEP11(2012)094},
Key = {fds320776}
}
@article{fds307828,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Cabrera, S and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De
Cecco, S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier,
L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field,
R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu,
S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis,
E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu,
T and Lockwitz, S and Lockyer, NS and Loginov, A and Lucchesi, D and Lueck,
J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak,
R and Maeshima, K and Makhoul, K and Maksimovic, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez,
T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Santi,
L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt,
M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stanitzki,
M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Turini, N and Ukegawa, F and Uozumi, S and Varganov, A and Vataga, E and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vogel, M and Volpi, G and Wagner, P and Wagner,
RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters,
D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK},
Title = {Search for a heavy toplike quark in pp collisions at
√s=1.96 TeV.},
Journal = {Physical review letters},
Volume = {107},
Number = {26},
Pages = {261801},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.107.261801},
Abstract = {We present the results of a search for pair production of a
heavy toplike (t') quark decaying to Wq final states using
data corresponding to an integrated luminosity of 5.6 fb(-1)
collected by the CDF II detector in pp collisions at
√s=1.96 TeV. We perform parallel searches for t'→Wb and
t'→Wq (where q is a generic down-type quark) in events
containing a lepton and four or more jets. By performing a
fit to the two-dimensional distribution of total transverse
energy versus reconstructed t' quark mass, we set upper
limits on the t't' production cross section and exclude a
standard model fourth-generation t' quark decaying to Wb
(Wq) with mass below 358 (340) GeV/c(2) at 95%
C.L.},
Doi = {10.1103/physrevlett.107.261801},
Key = {fds307828}
}
@article{fds307658,
Author = {Aaltonen, T and Adelman, J and Lvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F},
Title = {Search for a heavy vector boson decaying to two gluons in
pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.86.112002},
Abstract = {We present a search for a new heavy vector boson Z′ that
decays to gluons. Decays to on-shell gluons are suppressed,
leading to a dominant decay mode of Z′→g*g. We study the
case where the off-shell gluon g* converts to a pair of top
quarks, leading to a final state of tt̄g. In a sample of
events with exactly one charged lepton, large missing
transverse momentum and at least five jets, corresponding to
an integrated luminosity of 8.7fb-1 collected by the CDF II
detector, we find the data to be consistent with the
standard model. We set upper limits on the production cross
section times branching ratio of this chromophilic Z′ at
95% confidence level from 300 to 40 fb for Z′ masses
ranging from 400 to 1000GeV/c2, respectively. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.86.112002},
Key = {fds307658}
}
@article{fds307964,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey,
P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes,
D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani,
M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo,
KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin,
PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kusakabe, Y and Kwang, S and Laasanen,
AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlok, J and Movilla Fernandez and P and Mülmenstädt,
J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini,
M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura,
K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman,
M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino,
G and Pianori, E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Rekovic, V and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Saltó,
O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro,
A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker,
GL},
Title = {Search for a Higgs boson decaying to two W bosons at
CDF.},
Journal = {Physical review letters},
Volume = {102},
Number = {2},
Pages = {021802},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.102.021802},
Abstract = {We present a search for a Higgs boson decaying to two W
bosons in pp[over ] collisions at sqrt[s]=1.96 TeV
center-of-mass energy. The data sample corresponds to an
integrated luminosity of 3.0 fb;(-1) collected with the CDF
II detector. We find no evidence for production of a Higgs
boson with mass between 110 and 200 GeV/c;(2), and determine
upper limits on the production cross section. For the mass
of 160 GeV/c;(2), where the analysis is most sensitive, the
observed (expected) limit is 0.7 pb (0.9 pb) at 95% Bayesian
credibility level which is 1.7 (2.2) times the standard
model cross section.},
Doi = {10.1103/physrevlett.102.021802},
Key = {fds307964}
}
@article{fds307716,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta,
M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko, A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Ray, J and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro,
A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri,
F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shiraishi, S and Shochet, M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari,
M and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton,
O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov,
A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK},
Title = {Search for a Higgs boson in the diphoton final state in pp
collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {1},
Pages = {011801},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.108.011801},
Abstract = {A search for a narrow Higgs boson resonance in the diphoton
mass spectrum is presented based on data corresponding to
7.0 fb{-1} of integrated luminosity from pp collisions
at sqrt[s]=1.96 TeV collected by the CDF experiment. No
evidence of such a resonance is observed, and upper limits
are set on the cross section times branching ratio of the
resonant state as a function of Higgs boson mass. The limits
are interpreted in the context of the standard model and one
fermiophobic benchmark model where the data exclude
fermiophobic Higgs bosons with masses below
114 GeV/c{2} at a 95% Bayesian credibility
level.},
Doi = {10.1103/physrevlett.108.011801},
Key = {fds307716}
}
@article{fds307681,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M},
Title = {Search for a Higgs boson in the diphoton final state using
the full CDF data set from pp collisions at
s=1.96TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {717},
Number = {1-3},
Pages = {173-181},
Publisher = {Elsevier BV},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2012.08.051},
Abstract = {A search for a narrow Higgs boson resonance in the diphoton
mass spectrum is presented based on data corresponding to
10fb -1 of integrated luminosity collected by the CDF
experiment from proton-antiproton collisions at s=1.96TeV.
To increase the sensitivity of the search, we employ a
multivariate discriminant technique for the first time in
this channel at CDF. No evidence of signal is observed, and
upper limits are set on the cross section times branching
ratio of the resonant state as a function of the Higgs boson
mass. The limits are interpreted in the context of the
standard model with an expected (observed) limit on the
cross section times branching ratio of 9.9 (17.0) times the
standard model prediction at the 95% credibility level for a
Higgs boson mass of 125GeV/c 2. Moreover, a Higgs boson with
suppressed couplings to fermions is excluded for masses
below 114GeV/c 2 at the 95% credibility level. © 2012
Elsevier B.V.},
Doi = {10.1016/j.physletb.2012.08.051},
Key = {fds307681}
}
@article{fds308051,
Author = {Aaltonen, and T, and others},
Title = {Search for a high-mass diphoton state and limits on
Randall-Sundrum gravitons at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {17},
Pages = {171801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.171801},
Abstract = {e have performed a search for new particles which decay to
two photons using 1.2 fb-1 of integrated luminosity from
p[overline p] collisions at sqrt(s)=1.96 TeV collected using
the CDF II detector at the Fermilab Tevatron. We find the
diphoton mass spectrum to be in agreement with the standard
model expectation, and set limits on the cross section times
branching ratio for the Randall-Sundrum graviton, as a
function of diphoton mass. We subsequently derive lower
limits for the graviton mass of 230 GeV/c2 and 850 GeV/c2,
at the 95\% confidence level, for coupling parameters
(k/[overline M]Pl) of 0.01 and 0.1, respectively.},
Doi = {10.1103/physrevlett.99.171801},
Key = {fds308051}
}
@article{fds356786,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for a high-mass Higgs boson decaying to a W boson
pair in pp collisions at (Formula presented.) TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {1},
Pages = {1-66},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2016)032},
Abstract = {Abstract: A search for a high-mass Higgs boson H is
performed in the H → WW → ℓνℓν and H → WW →
ℓνqq decay channels using pp collision data corresponding
to an integrated luminosity of 20.3 fb−1 collected at
s=8(Formula presented.) TeV by the ATLAS detector at the
Large Hadron Collider. No evidence of a high-mass Higgs
boson is found. Limits on σH × BR(H → WW) as a function
of the Higgs boson mass mH are determined in three different
scenarios: one in which the heavy Higgs boson has a narrow
width compared to the experimental resolution, one for a
width increasing with the boson mass and modeled by the
complex-pole scheme following the same behavior as in the
Standard Model, and one for intermediate widths. The upper
range of the search is mH = 1500 GeV for the narrow-width
scenario and mH = 1000 GeV for the other two scenarios. The
lower edge of the search range is 200–300 GeV and depends
on the analysis channel and search scenario. For each signal
interpretation, individual and combined limits from the two
WW decay channels are presented. At mH = 1500 GeV, the
highest-mass point tested, σH × BR(H → WW) for a
narrow-width Higgs boson is constrained to be less than 22
fb and 6.6 fb at 95% CL for the gluon fusion and
vector-boson fusion production modes, respectively.[Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP01(2016)032},
Key = {fds356786}
}
@article{fds307600,
Author = {The ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Åsman, B and Asner, D and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu,
E and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y},
Title = {Search for a light charged Higgs boson in the decay channel
[Formula: see text] in [Formula: see text] events using
pp collisions at [Formula: see text] with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {73},
Number = {6},
Pages = {2465},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2465-z},
Abstract = {A search for a charged Higgs boson (<i>H</i><sup>+</sup>) in
[Formula: see text] decays is presented, where one of the
top quarks decays via <i>t</i>→<i>H</i><sup>+</sup><i>b</i>,
followed by <i>H</i><sup>+</sup>→ two jets ([Formula: see
text]). The other top quark decays to <i>Wb</i>, where the
<i>W</i> boson then decays into a lepton
(<i>e</i>/<i>μ</i>) and a neutrino. The data were recorded
in <i>pp</i> collisions at [Formula: see text] by the ATLAS
detector at the LHC in 2011, and correspond to an integrated
luminosity of 4.7 fb<sup>-1</sup>. With no observation of a
signal, 95 % confidence level (CL) upper limits are set on
the decay branching ratio of top quarks to charged Higgs
bosons varying between 5 % and 1 % for
<i>H</i><sup>+</sup> masses between 90 GeV and 150 GeV,
assuming [Formula: see text].},
Doi = {10.1140/epjc/s10052-013-2465-z},
Key = {fds307600}
}
@article{fds307698,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau,
T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B},
Title = {Search for a light Higgs boson decaying to long-lived weakly
interacting particles in proton-proton collisions at sqrt[s]
= 7 TeV with the ATLAS detector.},
Journal = {Physical review letters},
Volume = {108},
Number = {25},
Pages = {251801},
Year = {2012},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.108.251801},
Abstract = {A search for the decay of a light Higgs boson (120-140 GeV)
to a pair of weakly interacting, long-lived particles in
1.94 fb(-1) of proton-proton collisions at sqrt[s] = 7 TeV
recorded in 2011 by the ATLAS detector is presented. The
search strategy requires that both long-lived particles
decay inside the muon spectrometer. No excess of events is
observed above the expected background and limits on the
Higgs boson production times branching ratio to weakly
interacting, long-lived particles are derived as a function
of the particle proper decay length.},
Doi = {10.1103/physrevlett.108.251801},
Key = {fds307698}
}
@article{fds321119,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Erbacher, R and Errede, S and Esham,
B},
Title = {Search for a low-mass neutral Higgs boson with suppressed
couplings to fermions using events with multiphoton final
states},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112010},
Abstract = {A search for a Higgs boson with suppressed couplings to
fermions, hf, assumed to be the neutral, lower-mass partner
of the Higgs boson discovered at the Large Hadron Collider,
is reported. Such a Higgs boson could exist in extensions of
the standard model with two Higgs doublets, and could be
produced via pp→H±hf→W∗hfhf→4γ+X, where H± is a
charged Higgs boson. This analysis uses all events with at
least three photons in the final state from
proton-antiproton collisions at a center-of-mass energy of
1.96 TeV collected by the Collider Detector at Fermilab,
corresponding to an integrated luminosity of 9.2 fb-1. No
evidence of a signal is observed in the data. Values of
Higgs-boson masses between 10 and 100 GeV/c2 are excluded at
95% Bayesian credibility.},
Doi = {10.1103/PhysRevD.93.112010},
Key = {fds321119}
}
@article{fds307707,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar,
C and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and De Cecco and S and De Lorenzo and G and Dell'Orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Devoto, F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann,
JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia,
JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara,
K and Hare, D and Hare, M and Harr, RF and Hatakeyama, K and Hays, C and Heck,
M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker,
A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon,
EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim,
DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro,
P and Makhoul, K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Martínez-Ballarín,
R and Mastrandrea, P and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Squillacioti, P and Stancari, M and Stanitzki, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán,
P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán,
J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang,
T},
Title = {Search for a low-mass standard model Higgs boson in the ττ
decay channel in pp collisions at sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {18},
Pages = {181804},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.181804},
Abstract = {We report on a search for the standard model Higgs boson
decaying into pairs of τ leptons in pp collisions produced
by the Tevatron at sqrt[s]=1.96 TeV. The analyzed data
sample was recorded by the CDFII detector and corresponds to
an integrated luminosity of 6.0 fb(-1). The search is
performed in the final state with one τ decaying
leptonically and the second one identified through its
semihadronic decay. Since no significant excess is observed,
a 95% credibility level upper limit on the production cross
section times branching ratio to the ττ final state is set
for hypothetical Higgs boson masses between 100 and
150 GeV/c2. For a Higgs boson of 120 GeV/c2 the
observed (expected) limit is 14.6 (15.3) the predicted
value.},
Doi = {10.1103/physrevlett.108.181804},
Key = {fds307707}
}
@article{fds307550,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin,
JF},
Title = {Search for a multi-Higgs-boson cascade in W+W
-bb̄ events with the ATLAS detector in pp
collisions at √s = 8 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.89.032002},
Abstract = {A search is presented for new particles in an extension to
the Standard Model that includes a heavy Higgs boson (H0),
an intermediate charged Higgs-boson pair (H-), and a light
Higgs boson (h0). The analysis searches for events involving
the production of a single heavy neutral Higgs boson which
decays to the charged Higgs boson and a W boson, where the
charged Higgs boson subsequently decays into a W boson and
the lightest neutral Higgs boson decaying to a
bottom-antibottom-quark pair. Such a cascade results in a
W-boson pair and a bottom-antibottom-quark pair in the final
state. Events with exactly one lepton, missing transverse
momentum, and at least four jets are selected from a data
sample corresponding to an integrated luminosity of 20.3
fb-1, collected by the ATLAS detector in proton-proton
collisions at √s = 8 TeV at the LHC. The data are found to
be consistent with Standard Model predictions, and 95%
confidence-level upper limits are set on the product of
cross section and branching ratio. These limits range from
0.065 to 43 pb as a function of H0 and H- masses, with mh0
fixed at 125 GeV. © 2014 CERN, for the ATLAS
Collaboration.},
Doi = {10.1103/PhysRevD.89.032002},
Key = {fds307550}
}
@article{fds308089,
Author = {Abulencia, and A, and others},
Title = {Search for a neutral Higgs boson decaying to a W boson pair
in $p\bar{p}$ collisions at $\sqrt{s} =$
1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {8},
Pages = {081802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.97.081802},
Abstract = {We present the results of a search for standard model Higgs
boson production with decay to WW*, identified through the
leptonic final states e+e-nu-bar nu, e+/- mu-/+ nu-bar nu
and mu+ mu- nu-bar nu. This search uses 360 pb-1 of data
collected from p anti-p collisions at s**(1/2) = 1.96 TeV by
the upgraded Collider Detector at Fermilab (CDF II). We
observe no signal excess and set 95% confidence level upper
limits on the production cross section times branching ratio
for the Higgs boson to WW* or any new scalar particle with
similar decay products. These upper limits range from 5.5 to
3.2 pb for Higgs boson masses between 120 and 200
GeV/c2.},
Doi = {10.1103/physrevlett.97.081802},
Key = {fds308089}
}
@article{fds307882,
Author = {Aaltonen, and T, and al, E},
Title = {Search for a new heavy gauge boson ${W}^{$'${}}$ with event
signature $\mathrm{\text{electron}}+\mathrm{\text{missing}}$
transverse energy in $p\overline{p}$ collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {3},
Pages = {031102},
Publisher = {American Physical Society},
Year = {2011},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.83.031102},
Abstract = {We present a search for a new heavy charged vector boson
W′ decaying to an electron-neutrino pair in pp̄
collisions at a center-of-mass energy of 1.96 TeV. The data
were collected with the CDF II detector and correspond to an
integrated luminosity of 5.3fb-1. No significant excess
above the standard model expectation is observed and we set
upper limits on σ•B(W′→eν). Assuming standard model
couplings to fermions and the neutrino from the W′ boson
decay to be light, we exclude a W′ boson with mass less
than 1.12TeV/c2 at the 95% confidence level. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.031102},
Key = {fds307882}
}
@article{fds347476,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
Title = {Search for a new heavy gauge-boson resonance decaying into a
lepton and missing transverse momentum in 36 fb - 1 of
pp collisions at s = 13 TeV with the ATLAS
experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {5},
Pages = {401},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5877-y},
Abstract = {The results of a search for new heavy W ' bosons decaying to
an electron or muon and a neutrino using proton-proton
collision data at a centre-of-mass energy of s = 13 TeV
are presented. The dataset was collected in 2015 and 2016 by
the ATLAS experiment at the Large Hadron Collider and
corresponds to an integrated luminosity of 36.1 fb - 1 .
As no excess of events above the Standard Model prediction
is observed, the results are used to set upper limits on the
W ' boson cross-section times branching ratio to an electron
or muon and a neutrino as a function of the W ' mass.
Assuming a W ' boson with the same couplings as the Standard
Model <i>W</i> boson, W ' masses below 5.1 TeV are excluded
at the 95% confidence level.},
Doi = {10.1140/epjc/s10052-018-5877-y},
Key = {fds347476}
}
@article{fds375228,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Pandya, HD and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Castillo, FL and Costanza, F and Delmastro, M and Di
Ciaccio, L and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo
Martinez, N and Poddar, G and Sanchez Pineda and A and Sauvan, E and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Li, T and Marchiori, G and Nakkalil, K and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Wamorkar, T and Wang, R and Zhang, J and Cheu, E and Cui,
Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Tost,
M},
Title = {Search for a new pseudoscalar decaying into a pair of muons
in events with a top-quark pair at Formula Presented with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {108},
Number = {9},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.108.092007},
Abstract = {A search for a new pseudoscalar Formula Presented-boson
produced in events with a top-quark pair, where the Formula
Presented-boson decays into a pair of muons, is performed
using Formula Presented Formula Presented collision data
collected with the ATLAS detector at the LHC, corresponding
to an integrated luminosity of Formula Presented. The search
targets the final state where only one top quark decays to
an electron or muon, resulting in a signature with three
leptons Formula Presented and Formula Presented. No
significant excess of events above the Standard Model
expectation is observed and upper limits are set on two
signal models: Formula Presented and Formula Presented with
Formula Presented, Formula Presented, where Formula
Presented, in the mass ranges Formula Presented and Formula
Presented.},
Doi = {10.1103/PhysRevD.108.092007},
Key = {fds375228}
}
@article{fds313593,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM},
Title = {Search for a new resonance decaying to a W or
Z boson and a Higgs boson in the [Formula: see text]
final states with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {6},
Pages = {263},
Year = {2015},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3474-x},
Abstract = {A search for a new resonance decaying to a <i>W</i> or
<i>Z</i> boson and a Higgs boson in the [Formula: see text]
final states is performed using 20.3 fb[Formula: see text]
of <i>pp</i> collision data recorded at [Formula: see
text] 8 TeV with the ATLAS detector at the Large Hadron
Collider. The search is conducted by examining the
<i>WH</i> / <i>ZH</i> invariant mass distribution for a
localized excess. No significant deviation from the Standard
Model background prediction is observed. The results are
interpreted in terms of constraints on the Minimal Walking
Technicolor model and on a simplified approach based on a
phenomenological Lagrangian of Heavy Vector
Triplets.},
Doi = {10.1140/epjc/s10052-015-3474-x},
Key = {fds313593}
}
@article{fds356559,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
Abud, A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid,
OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios,
C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras,
D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella,
L},
Title = {Search for a right-handed gauge boson decaying into a
high-momentum heavy neutrino and a charged lepton in pp
collisions with the ATLAS detector at s=13
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {798},
Year = {2019},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2019.134942},
Abstract = {A search for a right-handed gauge boson WR, decaying into a
boosted right-handed heavy neutrino NR, in the framework of
Left-Right Symmetric Models is presented. It is based on
data from proton–proton collisions with a centre-of-mass
energy of 13 TeV collected by the ATLAS detector at the
Large Hadron Collider during the years 2015, 2016 and 2017,
corresponding to an integrated luminosity of 80 fb−1. The
search is performed separately for electrons and muons in
the final state. A distinguishing feature of the search is
the use of large-radius jets containing electrons.
Selections based on the signal topology result in smaller
background compared to the expected signal. No significant
deviation from the Standard Model prediction is observed and
lower limits are set in the WR and NR mass plane. Mass
values of the WR smaller than 3.8–5 TeV are excluded for
NR in the mass range 0.1–1.8 TeV.},
Doi = {10.1016/j.physletb.2019.134942},
Key = {fds356559}
}
@article{fds352202,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
Title = {Search for a scalar partner of the top quark in the
all-hadronic tt¯ plus missing transverse momentum final
state at √s=13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {8},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8102-8},
Abstract = {A search for direct pair production of scalar partners of
the top quark (top squarks or scalar third-generation
up-type leptoquarks) in the all-hadronic tt¯ plus missing
transverse momentum final state is presented. The analysis
of 139 fb - 1 of s=13 TeV proton–proton collision data
collected using the ATLAS detector at the LHC yields no
significant excess over the Standard Model background
expectation. To interpret the results, a supersymmetric
model is used where the top squark decays via
t~→t(∗)χ~10, with t(∗) denoting an on-shell
(off-shell) top quark and χ~10 the lightest neutralino.
Three specific event selections are optimised for the
following scenarios. In the scenario where mt~>mt+mχ~10,
top squark masses are excluded in the range 400–1250 GeV
for χ~10 masses below 200 GeV at 95% confidence level. In
the situation where mt~∼mt+mχ~10, top squark masses in
the range 300–630 GeV are excluded, while in the case
where mt~<mW+mb+mχ~10 (with mt~-mχ~10≥5 GeV),
considered for the first time in an ATLAS all-hadronic
search, top squark masses in the range 300–660 GeV are
excluded. Limits are also set for scalar third-generation
up-type leptoquarks, excluding leptoquarks with masses below
1240 GeV when considering only leptoquark decays into a top
quark and a neutrino.},
Doi = {10.1140/epjc/s10052-020-8102-8},
Key = {fds352202}
}
@article{fds356719,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for a scalar partner of the top quark in the jets
plus missing transverse momentum final state at √s=13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {12},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2017)085},
Abstract = {A search for pair production of a scalar partner of the top
quark in events with four or more jets plus missing
transverse momentum is presented. An analysis of 36.1 fb−1
of s=13 TeV proton-proton collisions collected using the
ATLAS detector at the LHC yields no significant excess over
the expected Standard Model background. To interpret the
results a simplified supersymmetric model is used where the
top squark is assumed to decay via t˜1→t(∗)χ˜10 and
t˜1→bχ˜1±→bW(∗)χ˜10, where χ10(χ1±) denotes
the lightest neutralino (chargino). Exclusion limits are
placed in terms of the top-squark and neutralino masses.
Assuming a branching ratio of 100% to tχ˜10, top-squark
masses in the range 450–1000 GeV are excluded for χ˜10
masses below 160 GeV. In the case where mt˜1∼mt+mχ˜10,
top-squark masses in the range 235–590 GeV are
excluded.},
Doi = {10.1007/JHEP12(2017)085},
Key = {fds356719}
}
@article{fds307832,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
Title = {Search for a standard model Higgs boson in the
H→ZZ→ℓ(+)ℓ(-)νν decay channel with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {107},
Number = {22},
Pages = {221802},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.107.221802},
Abstract = {A search for a heavy standard model Higgs boson decaying via
H→ZZ→→ℓ(+)ℓ(-)νν, where ℓ=e, μ, is presented.
It is based on proton-proton collision data at √s=7 TeV,
collected by the ATLAS experiment at the LHC in the first
half of 2011 and corresponding to an integrated luminosity
of 1.04 fb(-1). The data are compared to the expected
standard model backgrounds. The data and the background
expectations are found to be in agreement and upper limits
are placed on the Higgs boson production cross section over
the entire mass window considered; in particular, the
production of a standard model Higgs boson is excluded in
the region 340<m(H)<450 GeV at the 95% confidence
level.},
Doi = {10.1103/physrevlett.107.221802},
Key = {fds307832}
}
@article{fds307795,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D},
Title = {Search for a standard model Higgs boson in the
H→ZZ→ℓ+ℓ−νν¯ decay
channel using 4.7 fb−1 of √s=7 TeV data with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {717},
Number = {1-3},
Pages = {29-48},
Publisher = {Elsevier BV},
Year = {2012},
Month = {October},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.09.016},
Abstract = {A search for a Standard Model Higgs boson decaying via
H→ZZ→ℓ+ℓ−νν¯ where ℓ represents electrons or
muons, is presented. It is based on proton-proton collision
data at s=7 TeV, collected by the ATLAS experiment at the
LHC during 2011 and corresponding to an integrated
luminosity of 4.7 fb−1. The data agree with the expected
Standard Model backgrounds. Upper limits on the Higgs boson
production cross section are derived for Higgs boson masses
between 200 GeV and 600 GeV and the production of a Standard
Model Higgs boson with a mass in the range 319–558 GeV is
excluded at the 95% confidence level.},
Doi = {10.1016/j.physletb.2012.09.016},
Key = {fds307795}
}
@article{fds307785,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
NJ and Collins-Tooth, C and Collot, J and Colombo,
T},
Title = {Search for a Standard Model Higgs boson in the mass range
200-600GeV in the H→ZZ→ℓ+ℓ-qq̄ decay channel with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {717},
Number = {1-3},
Pages = {70-88},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.09.020},
Abstract = {A search for a heavy Standard Model Higgs boson decaying via
H→ZZ→ℓ+ℓ-qq̄, where ℓ=e or μ, is presented. The
search uses a data set of pp collisions at s=7TeV,
corresponding to an integrated luminosity of 4.7fb-1
collected in 2011 by the ATLAS detector at the CERN LHC. No
significant excess of events above the estimated background
is found. Upper limits at 95% confidence level on the
production cross section of a Higgs boson with a mass in the
range between 200 and 600GeV are derived. A Standard Model
Higgs boson with a mass in the range 300GeV≤mH≤322GeV or
353GeV≤mH≤410GeV is excluded at 95% CL. The
corresponding expected exclusion range is
351GeV≤mH≤404GeV at 95% CL. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.09.020},
Key = {fds307785}
}
@article{fds307942,
Author = {Aaltonen, T and others},
Title = {Search for a Standard Model Higgs Boson in WH→ℓvbb̅ in
pp̅ Collisions at sqrt[s] =1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {10},
Pages = {101802},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.101802},
Abstract = {We present a search for a standard model Higgs boson
produced in association with a W boson using 2.7 fb-1
of integrated luminosity of pp̅ collision data taken at
sqrt[s]=1.96 TeV. Limits on the Higgs boson production
rate are obtained for masses between 100 and
150 GeV/c2. Through the use of multivariate techniques,
the analysis achieves an observed (expected) 95% confidence
level upper limit of 5.6 (4.8) times the theoretically
expected production cross section for a standard model Higgs
boson with a mass of 115 GeV/c2.},
Doi = {10.1103/physrevlett.103.101802},
Key = {fds307942}
}
@article{fds347460,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Bakshi
Gupta, D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov,
A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin,
DL and Bristow, TM and Britton, D and Britzger, D and Brock, I and Brock,
R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran,
J},
Title = {Search for a Structure in the B_{s}^{0}π^{±} Invariant
Mass Spectrum with the ATLAS Experiment.},
Journal = {Physical review letters},
Volume = {120},
Number = {20},
Pages = {202007},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.120.202007},
Abstract = {A search for the narrow structure, X(5568), reported by the
D0 Collaboration in the decay sequence X→B_{s}^{0}π^{±},
B_{s}^{0}→J/ψϕ, is presented. The analysis is based on a
data sample recorded with the ATLAS detector at the LHC
corresponding to 4.9 fb^{-1} of pp collisions at 7 TeV
and 19.5 fb^{-1} at 8 TeV. No significant signal was
found. Upper limits on the number of signal events, with
properties corresponding to those reported by D0, and on the
X production rate relative to B_{s}^{0} mesons, ρ_{X}, were
determined at 95% confidence level. The results are
N(X)<382 and ρ_{X}<0.015 for B_{s}^{0} mesons with
transverse momenta above 10 GeV, and N(X)<356 and
ρ_{X}<0.016 for transverse momenta above 15 GeV. Limits
are also set for potential B_{s}^{0}π^{±} resonances in
the mass range 5550 to 5700 MeV.},
Doi = {10.1103/physrevlett.120.202007},
Key = {fds347460}
}
@article{fds307666,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer,
F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
Harpaz, S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal,
M},
Title = {Search for a supersymmetric partner to the top quark in
final states with jets and missing transverse momentum at
sqrt[s] = 7 TeV with the ATLAS detector.},
Journal = {Physical review letters},
Volume = {109},
Number = {21},
Pages = {211802},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.109.211802},
Abstract = {A search for direct pair production of supersymmetric top
squarks (t(1)) is presented, assuming the t(1) decays into a
top quark and the lightest supersymmetric particle,
χ(1)(0), and that both top quarks decay to purely hadronic
final states. A total of 16 (4) events are observed compared
to a predicted standard model background of
13.5(-3.6)(+3.7)(4.4(-1.3)(+1.7)) events in two signal
regions based on ∫Ldt = 4.7 fb(-1) of pp collision data
taken at sqrt[s] = 7 TeV with the ATLAS detector at the LHC.
An exclusion region in the t(1) versus χ(1)(0) mass plane
is evaluated: 370<m(t)(1)}<465 GeV is excluded for
m(χ)(1)(0) ~ 0 GeV while m(t)(1) = 445 GeV is excluded for
m(χ)(1)(0) ≤ 50 GeV.},
Doi = {10.1103/physrevlett.109.211802},
Key = {fds307666}
}
@article{fds307609,
Author = {Aaltonen, T and Adelman, J and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas,
W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro,
M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi,
A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harr,
RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon,
M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang,
D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Johnstone, A and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Rao, K and Redondo, I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Truong, A and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund,
AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Search for a two-Higgs-boson doublet using a simplified
model in pp collisions at sqrt[s] = 1.96
TeV.},
Journal = {Physical review letters},
Volume = {110},
Number = {12},
Pages = {121801},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.110.121801},
Abstract = {We present a search for new particles in an extension to the
standard model that includes a heavy Higgs boson (H(0)), a
lighter charged Higgs boson (H(±)), and an even lighter
Higgs boson h(0), with decays leading to a W-boson pair and
a bottom-antibottom quark pair in the final state. We use
events with exactly one lepton, missing transverse momentum,
and at least four jets in data corresponding to an
integrated luminosity of 8.7 fb(-1) collected by the CDF II
detector in proton-antiproton collisions at sqrt[s]= 1.96
TeV. We find the data to be consistent with standard model
predictions and report the results in terms of a simplified
Higgs-cascade-decay model, setting 95% confidence level
upper limits on the product of cross section and branching
fraction from 1.3 pb to 15 fb as a function of H(0) and
H(±) masses for m(h)(0) = 126 GeV/c(2).},
Doi = {10.1103/physrevlett.110.121801},
Key = {fds307609}
}
@article{fds307844,
Author = {Aaltonen, and T, and al, E},
Title = {Search for a Very Light ${CP}$-Odd {H}iggs Boson in Top
Quark Decays from $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {3},
Pages = {031801},
Publisher = {American Physical Society},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.031801},
Abstract = {We present the results of a search for a very light CP-odd
Higgs boson a(1)(0) originating from top quark decays t →
H(±)b → W(±(*)) a(1)(0)b, and subsequently decaying into
τ+ τ-. Using a data sample corresponding to an integrated
luminosity of 2.7 fb(-1) collected by the CDF II
detector in pp collisions at 1.96 TeV, we perform a search
for events containing a lepton, three or more jets, and an
additional isolated track with transverse momentum in the
range 3 to 20 GeV/c. Observed events are consistent
with background sources, and 95% C.L. limits are set on the
branching ratio of t → H(±)b for various masses of H(±)
and a(1)(0).},
Doi = {10.1103/PhysRevLett.107.031801},
Key = {fds307844}
}
@article{fds356702,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for additional heavy neutral Higgs and gauge bosons
in the ditau final state produced in 36 fb−1 of
pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {1},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2018)055},
Abstract = {A search for heavy neutral Higgs bosons and Z′ bosons is
performed using a data sample corresponding to an integrated
luminosity of 36.1 fb−1 from proton-proton collisions at
s=13 TeV recorded by the ATLAS detector at the LHC during
2015 and 2016. The heavy resonance is assumed to decay to
τ+τ− with at least one tau lepton decaying to final
states with hadrons and a neutrino. The search is performed
in the mass range of 0.2-2.25 TeV for Higgs bosons and
0.2-4.0 TeV for Z′ bosons. The data are in good agreement
with the background predicted by the Standard Model. The
results are interpreted in benchmark scenarios. In the
context of the hMSSM scenario, the data exclude tan β > 1.0
for mA = 0.25 TeV and tan β > 42 for mA = 1.5 TeV at the
95% confidence level. For the Sequential Standard Model,
ZSSM′ with mZ′ < 2.42 TeV is excluded at 95% confidence
level, while ZNU′ with mZ ′ < 2.25 TeV is excluded for
the non-universal G(221) model that exhibits enhanced
couplings to third-generation fermions.},
Doi = {10.1007/JHEP01(2018)055},
Key = {fds356702}
}
@article{fds321129,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {Search for an additional, heavy Higgs boson in the [Formula:
see text] decay channel at [Formula: see text] in [Formula:
see text] collision data with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {45},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3820-z},
Abstract = {A search is presented for a high-mass Higgs boson in the
[Formula: see text], [Formula: see text], [Formula: see
text], and [Formula: see text] decay modes using the ATLAS
detector at the CERN Large Hadron Collider. The search uses
proton-proton collision data at a centre-of-mass energy of
8 TeV corresponding to an integrated luminosity of
20.3 fb[Formula: see text]. The results of the search are
interpreted in the scenario of a heavy Higgs boson with a
width that is small compared with the experimental mass
resolution. The Higgs boson mass range considered extends up
to [Formula: see text] for all four decay modes and down to
as low as 140 [Formula: see text], depending on the decay
mode. No significant excess of events over the Standard
Model prediction is found. A simultaneous fit to the four
decay modes yields upper limits on the production
cross-section of a heavy Higgs boson times the branching
ratio to [Formula: see text] boson pairs. 95 % confidence
level upper limits range from 0.53 pb at [Formula: see
text] GeV to 0.008 pb at [Formula: see text] GeV for the
gluon-fusion production mode and from 0.31 pb at [Formula:
see text] GeV to 0.009 pb at [Formula: see text] GeV for
the vector-boson-fusion production mode. The results are
also interpreted in the context of Type-I and Type-II
two-Higgs-doublet models.},
Doi = {10.1140/epjc/s10052-015-3820-z},
Key = {fds321129}
}
@article{fds356701,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for an invisibly decaying Higgs boson or dark matter
candidates produced in association with a Z boson in pp
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {776},
Pages = {318-337},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2017.11.049},
Abstract = {A search for an invisibly decaying Higgs boson or dark
matter candidates produced in association with a
leptonically decaying Z boson in proton–proton collisions
at s=13 TeV is presented. This search uses 36.1 fb−1 of
data collected by the ATLAS experiment at the Large Hadron
Collider. No significant deviation from the expectation of
the Standard Model backgrounds is observed. Assuming the
Standard Model ZH production cross-section, an observed
(expected) upper limit of 67% (39%) at the 95% confidence
level is set on the branching ratio of invisible decays of
the Higgs boson with mass mH=125 GeV. The corresponding
limits on the production cross-section of the ZH process
with the invisible Higgs boson decays are also presented.
Furthermore, exclusion limits on the dark matter candidate
and mediator masses are reported in the framework of
simplified dark matter models.},
Doi = {10.1016/j.physletb.2017.11.049},
Key = {fds356701}
}
@article{fds356762,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for anomalous electroweak production of WW /WZ in
association with a high-mass dijet system in pp collisions
at s =8 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {95},
Number = {3},
Year = {2017},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.95.032001},
Abstract = {A search is presented for anomalous quartic gauge boson
couplings in vector-boson scattering. The data for the
analysis correspond to 20.2 fb-1 of s=8 TeV pp collisions
and were collected in 1972 by the ATLAS experiment at the
Large Hadron Collider. The search looks for the production
of WW or WZ boson pairs accompanied by a high-mass dijet
system, with one W decaying leptonically and a W or Z
decaying hadronically. The hadronically decaying W/Z is
reconstructed as either two small-radius jets or one
large-radius jet using jet substructure techniques.
Constraints on the anomalous quartic gauge boson coupling
parameters α4 and α5 are set by fitting the transverse
mass of the diboson system, and the resulting 95% confidence
intervals are -0.024<α4<0.030 and -0.028<α5<0.033.},
Doi = {10.1103/PhysRevD.95.032001},
Key = {fds356762}
}
@article{fds352492,
Author = {Acosta, and D, and others},
Title = {Search for anomalous kinematics in t anti-t dilepton events
at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {95},
Number = {2},
Pages = {022001},
Year = {2005},
url = {http://dx.doi.org/10.1103/physrevlett.95.022001},
Abstract = {http://arxiv.org/abs/hep-ex/0412042},
Doi = {10.1103/physrevlett.95.022001},
Key = {fds352492}
}
@article{fds308149,
Author = {Acosta, and D, and others},
Title = {Search for anomalous production of diphoton events with
missing transverse energy at CDF and limits on gauge-
mediated supersymmetry-breaking models},
Journal = {Phys. Rev.},
Volume = {D71},
Number = {3},
Pages = {031104},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.031104},
Abstract = {http://arxiv.org/abs/hep-ex/0410053},
Doi = {10.1103/PhysRevD.71.031104},
Key = {fds308149}
}
@article{fds307978,
Author = {Aaltonen, T and others},
Title = {Search for anomalous production of events with a photon,
jet, b-quark jet, and missing transverse
energy},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {5},
Pages = {052003},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.052003},
Abstract = {We present a signature-based search for the anomalous
production of events containing a photon, two jets, of which
at least one is identified as originating from a b quark,
and missing transverse energy (E̸T). The search uses data
corresponding to 2.0 fb-1 of integrated luminosity from
pp̅ collisions at a center-of-mass energy of
sqrt[s]=1.96 TeV, collected with the CDF II detector at
the Fermilab Tevatron. From 6.697 47×106 events with a
photon candidate with transverse energy ET>25 GeV,
we find 617 events with E̸T>25 GeV and two or more
jets with ET>15 GeV, at least one identified as
originating from a b quark, versus an expectation of 607
± 113 events. Increasing the requirement on E̸T to
50 GeV, we find 28 events versus an expectation of 30
± 11 events. We find no indications of
non-standard-model phenomena.},
Doi = {10.1103/PhysRevD.80.052003},
Key = {fds307978}
}
@article{fds307927,
Author = {Aaltonen, and T, and others},
Title = {Search for anomalous production of events with two photons
and additional energetic objects at CDF},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {5},
Pages = {052005},
Publisher = {American Physical Society},
Year = {2010},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.82.052005},
Abstract = {We present results of a search for anomalous production of
two photons together with an electron, muon, τ lepton,
missing transverse energy, or jets using pp̄ collision data
from 1.1-2.0fb-1 of integrated luminosity collected by the
Collider Detector at Fermilab (CDF). The event yields and
kinematic distributions are examined for signs of new
physics without favoring a specific model of new physics.
The results are consistent with the standard model
expectations. The search employs several new analysis
techniques that significantly reduce instrumental
backgrounds in channels with an electron and missing
transverse energy. © 2010 The American Physical
Society.},
Doi = {10.1103/PhysRevD.82.052005},
Key = {fds307927}
}
@article{fds308059,
Author = {Abulencia, and A, and others},
Title = {Search for anomalous production of multi-lepton events in $p
\bar{p}$ collisions at $\sqrt{s}$ = 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {13},
Pages = {131804},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.131804},
Abstract = {We report a search for the anomalous production of events
with multiple charged leptons in p[overline p] collisions at
sqrt(s)=1.96 TeV using a data sample corresponding to an
integrated luminosity of 346 pb-1 collected by the CDF II
detector at the Fermilab Tevatron. The search is divided
into three-lepton and four-or-more-lepton data samples. We
observe six events in the three-lepton sample and zero
events in the >=4-lepton sample. Both numbers of events are
consistent with standard model background expectations.
Within the framework of an R-parity-violating supergravity
model, the results are interpreted as mass limits on the
lightest neutralino (chi-tilde10) and chargino
(chi-tilde1[plus-minus]) particles. For one particular
choice of model parameters, the limits are
M(chi-tilde10)>110 GeV/c2 and M(chi-tilde1[plus-minus])>203
GeV/c2 at 95\% confidence level; the variation of these mass
limits with model parameters is presented.},
Doi = {10.1103/physrevlett.98.131804},
Key = {fds308059}
}
@article{fds307818,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Search for anomalous production of multiple leptons in
association with W and Z bosons at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.85.092001},
Abstract = {This paper presents a search for anomalous production of
multiple low-energy leptons in association with a W or Z
boson using events collected at the CDF experiment
corresponding to 5.1fb -1 of integrated luminosity. This
search is sensitive to a wide range of topologies with
low-momentum leptons, including those with the leptons near
one another. The observed rates of production of additional
electrons and muons are compared with the standard model
predictions. No indications of phenomena beyond the standard
model are found. A 95% confidence level limit is presented
on the production cross section for a benchmark model of
supersymmetric hidden-valley Higgs production. Particle
identification efficiencies are also provided to enable the
calculation of limits on additional models. © 2012 American
Physical Society.},
Doi = {10.1103/PhysRevD.85.092001},
Key = {fds307818}
}
@article{fds307659,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram,
N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
M},
Title = {Search for anomalous production of prompt like-sign lepton
pairs at √s =7 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {12},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP12(2012)007},
Abstract = {An inclusive search for anomalous production of two prompt,
isolated leptons with the same electric charge is presented.
The search is performed in a data sample corresponding to
4.7 fb-1 of integrated luminosity collected in 2011 at √s
=7 TeV with the ATLAS detector at the LHC. Pairs of leptons
(e± e±, e± μ ±, and μ ± μ ±) with large transverse
momentum are selected, and the dilepton invariant mass
distribution is examined for any deviation from the Standard
Model expectation. No excess is found, and upper limits on
the production cross section of like-sign lepton pairs from
physics processes beyond the Standard Model are placed as a
function of the dilepton invariant mass within a fiducial
region close to the experimental selection criteria. The 95%
confidence level upper limits on the cross section of
anomalous e± e ±, e± μ ±, or μ ± μ ± production
range between 1.7 fb and 64 fb depending on the dilepton
mass and flavour combination. © 2012 Cern for the benefit
of the ATLAS collaboration.},
Doi = {10.1007/JHEP12(2012)007},
Key = {fds307659}
}
@article{fds307738,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for anomalous production of prompt like-sign muon
pairs and constraints on physics beyond the standard model
with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.85.032004},
Abstract = {An inclusive search for anomalous production of two prompt,
isolated muons with the same electric charge is presented.
The search is performed in a data sample corresponding to
1.6fb-1 of integrated luminosity collected in 2011 at
√s=7TeV with the ATLAS detector at the LHC. Muon pairs are
selected by requiring two isolated muons of the same
electric charge with p T>20GeV and |η|<2.5. Minimal
requirements are placed on the rest of the event activity.
The distribution of the invariant mass of the muon pair
m(μμ) is found to agree well with the background
expectation. Upper limits on the cross section for anomalous
production of two muons with the same electric charge are
placed as a function of m(μμ) within a fiducial region
defined by the event selection. The fiducial cross-section
limit constrains the like-sign top-quark pair-production
cross section to be below 3.7pb at 95% confidence level. The
data are also analyzed to search for a narrow like-sign
dimuon resonance as predicted for e.g. doubly charged Higgs
bosons (H ±). Assuming pair production of H± bosons and a
branching ratio to muons of 100% (33%), this analysis
excludes masses below 355 (244)GeV and 251 (209)GeV for H±
bosons coupling to left-handed and right-handed fermions,
respectively. © 2012 CERN. Published by the American
Physical Society under the terms of the uri
xlink:href=http://creativecommons.org/licenses/by/3.0/Creative
Commons Attribution 3.0 License. Further distribution of
this work must maintain attribution to the author(s) and the
published article's title, journal citation, and DOI. ©
2012 American Physical Society.},
Doi = {10.1103/PhysRevD.85.032004},
Key = {fds307738}
}
@article{fds310295,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for anomalous production of prompt same-sign lepton
pairs and pair-produced doubly charged Higgs bosons with s
=8 TeV pp collisions using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {3},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP03(2015)041},
Abstract = {Abstract: A low-background inclusive search for new physics
in events with same-sign dileptons is presented. The search
uses proton-proton collisions corresponding to 20.3 fb−1
of integrated luminosity taken in 2012 at a centre-of-mass
energy of 8 TeV with the ATLAS detector at the LHC. Pairs of
isolated leptons with the same electric charge and large
transverse momenta of the type e±e±, e±μ±, and μ±μ±
are selected and their invariant mass distribution is
examined. No excess of events above the expected level of
Standard Model background is found. The results are used to
set upper limits on the cross-sections for processes beyond
the Standard Model. Limits are placed as a function of the
dilepton invariant mass within a fiducial region
corresponding to the signal event selection criteria.
Exclusion limits are also derived for a specific model of
doubly charged Higgs boson production.[Figure not available:
see fulltext.]},
Doi = {10.1007/JHEP03(2015)041},
Key = {fds310295}
}
@article{fds308114,
Author = {Abulencia, and A, and others},
Title = {Search for anomalous semileptonic decay of heavy flavor
hadrons produced in association with a W boson at CDF
II},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {5},
Pages = {051101},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.051101},
Abstract = {We present a search for anomalous semileptonic decays of
heavy flavor hadrons produced in association with a W boson,
in proton-antiproton collisions at s**(1/2) = 1.96 TeV. We
use 162 pb-1 of data collected with the CDF II detector at
the Fermilab Tevatron Collider. We select events with one W
boson and at least one jet with an identified secondary
vertex. In the jets with a secondary vertex we look for a
semileptonic decay to a muon. We compare the number of jets
with both a secondary vertex and a semileptonic decay, and
the kinematic properties of these jets, with the standard
model expectation, and we set limits on the production cross
section of a B-like hadron with an anomalously high
semileptonic branching ratio.},
Doi = {10.1103/PhysRevD.73.051101},
Key = {fds308114}
}
@article{fds307825,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A},
Title = {Search for anomaly-mediated supersymmetry breaking with the
ATLAS detector based on a disappearing-track signature in pp
collisions at √s=7 TeV},
Journal = {European Physical Journal C},
Volume = {72},
Number = {4},
Pages = {1-20},
Publisher = {Springer Nature},
Year = {2012},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-1993-2},
Abstract = {In models of anomaly-mediated supersymmetry breaking (AMSB),
the lightest chargino is predicted to have a lifetime long
enough to be detected in collider experiments. This letter
explores AMSB scenarios in pp collisions at (Formula
Presented) = 7 TeV by attempting to identify decaying
charginos which result in tracks that appear to have few
associated hits in the outer region of the tracking system.
The search was based on data corresponding to an integrated
luminosity of 1.02 fb−1collected with the ATLAS detector
in 2011. The pT spectrum of candidate tracks is found to be
consistent with the expectation from Standard Model
background processes and constraints on the lifetime and the
production cross section were obtained. In the minimal AMSB
framework with m3/2< 32 TeV, m0< 1.5 TeV, tanβ = 5 and μ >
0, a chargino having mass below 92 GeV and a lifetime
between 0.5 ns and 2 ns is excluded at 95 % confidence
level.},
Doi = {10.1140/epjc/s10052-012-1993-2},
Key = {fds307825}
}
@article{fds356699,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for B - L R-parity-violating top squarks in √s=13
TeV pp collisions with the ATLAS experiment},
Journal = {Physical Review D},
Volume = {97},
Number = {3},
Year = {2018},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.97.032003},
Abstract = {A search is presented for the direct pair production of the
stop, the supersymmetric partner of the top quark, that
decays through an R-parity-violating coupling to a final
state with two leptons and two jets, at least one of which
is identified as a b-jet. The data set corresponds to an
integrated luminosity of 36.1 fb-1 of proton-proton
collisions at a center-of-mass energy of √s= 13 TeV,
collected in 2015 and 2016 by the ATLAS detector at the LHC.
No significant excess is observed over the Standard Model
background, and exclusion limits are set on stop pair
production at a 95% confidence level. Lower limits on the
stop mass are set between 600 GeV and 1.5 TeV for branching
ratios above 10% for decays to an electron or muon and a
b-quark.},
Doi = {10.1103/PhysRevD.97.032003},
Key = {fds356699}
}
@article{fds308165,
Author = {Acousta, D and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Calafiura, P and Campanelli, M and Campbell, M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat,
C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de
Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Dininno, M and De Pedis,
D and Derwent, PF and Devlin, T and Dionisi, C and Dittmann, JR and Doksus,
P and Dominguez, A and Donati, S and Donega, M and D'Onnofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy, N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan,
G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester,
S and Foster, GW and Franklin, M and Frisch, H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Gondcharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra,
Y and Goulianos, K and Gresele, A and Grosso-Pilcher, C and Guenther, M and Guimaraes da Costa and J and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans,
D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Karagoz Unel and M and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Kongisberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin,
CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lukens, P and Lyons, L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martiínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and McNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller, JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Moulik, T and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, A-S and Nigmanov, T and Nodulman, L and Oesterberg, K and Ogawa, T and Oh, S and Oh, YD and Ohsugi, T and Okusawa,
T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pitts, KT and Plager, C and Pompos, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio,
S and Ratnikov, F and Ray, H and Reichold, A and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert, K and Ristori, L and Robertson,
WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Schemitz, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Sfiligoi, I and Shears,
T and Scribano, A and Scuri, F and Sefov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Shapiro, MD and Shepard, PF and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siket, M and Sill, A and Sinervo, P and Sisakyan, A and Skiba, A and Slaughter, AJ and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Somalwar, SV and Spalding, J and Spezziga, M and Spiegel, L and Spinella, F and Spiropulu, M and Squillacioti, P and Stadie,
H},
Title = {Search for B0s-->micro+micro- and B0d-->micro+micro- decays
in pp collisions at square root s = 1.96
TeV.},
Journal = {Physical review letters},
Volume = {93},
Number = {3},
Pages = {032001},
Year = {2004},
Month = {July},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.93.032001},
Abstract = {We report on a search for B(0)(s)-->micro(+)micro(-) and
B(0)(d)-->micro(+)micro(-) decays in pp collisions at square
root of s=1.96 TeV using 171 pb(-1) of data collected by the
CDF II experiment at the Fermilab Tevatron Collider. The
decay rates of these rare processes are sensitive to
contributions from physics beyond the standard model. One
event survives all our selection requirements, consistent
with the background expectation. We derive branching ratio
limits of B(B(0)(s)-->micro(+)micro(-))<5.8x10(-7) and
B(B(0)(d)-->micro(+)micro(-))<1.5x10(-7) at 90% confidence
level.},
Doi = {10.1103/physrevlett.93.032001},
Key = {fds308165}
}
@article{fds308154,
Author = {al, DAE},
Title = {Search for B0s-->µ+µ- and B0d-->µ+µ- Decays in pp-bar
Collisions at sqrt[s]=1.96 TeV},
Journal = {Physical Review Letters},
Volume = {93},
Number = {5},
Pages = {032001},
Publisher = {American Physical Society (APS)},
Year = {2004},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.72.051104},
Abstract = {We report on a search for B0s-->µ+µ- and B0d-->µ+µ-
decays in pp-bar collisions at sqrt[s]=1.96 TeV using 171
pb-1 of data collected by the CDF II experiment at the
Fermilab Tevatron Collider. The decay rates of these rare
processes are sensitive to contributions from physics beyond
the standard model. One event survives all our selection
requirements, consistent with the background expectation. We
derive branching ratio limits of B(B0s--
>µ+µ-)µ+µ-)},
Doi = {10.1103/PhysRevD.72.051104},
Key = {fds308154}
}
@article{fds321085,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel,
C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and El
Moursli, RC and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Search for bottom squark pair production in proton-proton
collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {547},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4382-4},
Abstract = {The result of a search for pair production of the
supersymmetric partner of the Standard Model bottom quark
([Formula: see text]) is reported. The search uses
3.2 fb[Formula: see text] of <i>pp</i> collisions at
[Formula: see text] TeV collected by the ATLAS experiment
at the Large Hadron Collider in 2015. Bottom squarks are
searched for in events containing large missing transverse
momentum and exactly two jets identified as originating from
<i>b</i>-quarks. No excess above the expected Standard Model
background yield is observed. Exclusion limits at 95 %
confidence level on the mass of the bottom squark are
derived in phenomenological supersymmetric
<i>R</i>-parity-conserving models in which the [Formula: see
text] is the lightest squark and is assumed to decay
exclusively via [Formula: see text], where [Formula: see
text] is the lightest neutralino. The limits significantly
extend previous results; bottom squark masses up to 800
(840) GeV are excluded for the [Formula: see text] mass
below 360 (100) GeV whilst differences in mass above
100 GeV between the [Formula: see text] and the [Formula:
see text] are excluded up to a [Formula: see text] mass of
500 GeV.},
Doi = {10.1140/epjc/s10052-016-4382-4},
Key = {fds321085}
}
@article{fds308220,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Bross, A and Buchholz, D and Burtovoi,
VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Signore,
KD and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Loreto, GD and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum,
E},
Title = {Search for bottom squarks in [formula presented] collisions
at [formula presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {3},
Pages = {1-5},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.60.031101},
Abstract = {We report on a search for bottom squarks (Formula presented)
produced in (Formula presented) collisions at (Formula
presented) using the DØ detector at Fermilab. Bottom
squarks are assumed to be produced in pairs and to decay to
the lightest supersymmetric particle (LSP) and a b quark
with a branching fraction of 100%. The LSP is assumed to be
the lightest neutralino and stable. We set limits on the
production cross section as a function of (Formula
presented) mass and LSP mass. © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevD.60.031101},
Key = {fds308220}
}
@article{fds356557,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Search for bottom-squark pair production with the ATLAS
detector in final states containing Higgs bosons, b-jets and
missing transverse momentum},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {12},
Year = {2019},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2019)060},
Abstract = {The result of a search for the pair production of the
lightest supersymmetric partner of the bottom quark (b˜ 1)
using 139 fb−1 of proton-proton data collected at s = 13
TeV by the ATLAS detector is reported. In the supersymmetric
scenarios considered both of the bottom-squarks decay into a
b-quark and the second-lightest neutralino, b˜1→b+χ˜20.
Each χ˜20 is assumed to subsequently decay with 100%
branching ratio into a Higgs boson (h) like the one in the
Standard Model and the lightest neutralino:
χ˜20→h+χ˜10. The χ˜10 is assumed to be the lightest
supersymmetric particle (LSP) and is stable. Two signal mass
configurations are targeted: the first has a constant LSP
mass of 60 GeV; and the second has a constant mass
difference between the χ˜20 and χ˜10 of 130 GeV. The
final states considered contain no charged leptons, three or
more b-jets, and large missing transverse momentum. No
significant excess of events over the Standard Model
background expectation is observed in any of the signal
regions considered. Limits at the 95% confidence level are
placed in the supersymmetric models considered, and
bottom-squarks with mass up to 1.5 TeV are excluded. [Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP12(2019)060},
Key = {fds356557}
}
@article{fds308036,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar,
P and Behari, S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and De
Lorenzo, G and Dell'orso, M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di
Ruzza, B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza,
C and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt,
J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein,
S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis,
E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson,
W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Koay, SA and Kondo,
K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marino, C and Marino, CP and Martin,
A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín,
R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Mehtala, P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello,
M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan Griso and S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna,
G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria,
A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J},
Title = {Search for Bs0 --> micro+ micro- and B0 --> micro+ micro-
decays with 2 fb-1 of pp collisions.},
Journal = {Physical review letters},
Volume = {100},
Number = {10},
Pages = {101802},
Year = {2008},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.100.101802},
Abstract = {We have performed a search for B(s)(0) --> micro(+) micro(-)
and B(0) --> micro(+) micro(-) decays in pp collisions at
square root s = 1.96 TeV using 2 fb(-1) of integrated
luminosity collected by the CDF II detector at the Fermilab
Tevatron Collider. The observed number of B(s)(0) and B0
candidates is consistent with background expectations. The
resulting upper limits on the branching fractions are
B(B(s)0) --> micro(+) micro(-)) <5.8 x 10(-8) and B(B(0) -->
micro(+) micro(-))<1.8 x 10(-8) at 95% C.L.},
Doi = {10.1103/physrevlett.100.101802},
Key = {fds308036}
}
@article{fds313579,
Author = {Aaltonen, T and González, BÁ and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Almenar, CC and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and Barbaro, PD and Cecco, SD and Lorenzo, GD and Dell'orso, M and Deluca,
C and Demortier, L and Deng, J and Deninno, M and Devoto, F and D'errico,
M and Canto, AD and Ruzza, BD and Dittmann, JR and D'onofrio, M and Donati,
S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, D and Errede, S and Ershaidat, N and Eusebi, R and Fang, HC and Farrington, S and Feindt, M and Fernandez,
JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank,
MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Galyardt, J and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hidas, D and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha,
MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum,
W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirby, M and Klimenko, S and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee,
E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, CJ and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, Q and Liu, T and Lockwitz,
S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Makhoul,
K and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, C and Martínez, M and Martínez-Ballarín, R and Mastrandrea, P and Mattson, ME and Mazzanti, P and Mcfarland, KS and Mcintyre, P and Mcnulty, R and Mehta, A and Mehtala, P and Menzione, A and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Fernandez, PM and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse,
E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava,
R and Ortolan, L and Griso, SP and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Potamianos, K and Poukhov, O and Prokoshin, F and Pronko,
A and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Rescigno,
M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodrigo,
T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rubbo, F and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sartori, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet,
M and Shreyber, I and Simonenko, A and Sinervo, P and Sissakian, A and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Somalwar, S and Sorin, V and Sperka, D and Squillacioti, P and Stancari, M and Stanitzki, M and Denis, RS and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Ttito-Guzmán, P and Tkaczyk, S and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Tu, Y and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Weinberger, M and Wester, WC and Whitehouse, B and Whiteson, D and Wicklund, AB and Wicklund, E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamaoka, J and Yang, T and Yang, UK and Yang, YC},
Title = {Search for Bs0→μ+μ- and
B0→μ+μ- decays with CDF
II},
Journal = {Physical Review Letters},
Volume = {107},
Number = {19},
Pages = {191801},
Year = {2011},
url = {http://www.ncbi.nlm.nih.gov/pubmed/22181596},
Abstract = {A search has been performed for Bs0→μ+μ- and B0→μ+μ-
decays using 7fb-1 of integrated luminosity collected by the
CDF II detector at the Fermilab Tevatron collider. The
observed number of B0 candidates is consistent with
background-only expectations and yields an upper limit on
the branching fraction of B(B0→μ+μ-)<6.0×10-9 at 95%
confidence level. We observe an excess of Bs0 candidates.
The probability that the background processes alone could
produce such an excess or larger is 0.27%. The probability
that the combination of background and the expected standard
model rate of Bs0→μ+μ- could produce such an excess or
larger is 1.9%. These data are used to determine
B(Bs0→μ+μ-)=(1.8-0.9+1.1)×10 -8 and provide an upper
limit of B(Bs0→μ+μ -)<4.0×10-8 at 95% confidence
level. © 2011 American Physical Society.},
Doi = {10.1103/PhysRevLett.107.191801},
Key = {fds313579}
}
@article{fds307607,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Search for Bs0→μ+μ- and
B0→μ+μ- decays with the full CDF
Run II data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.87.072003},
Abstract = {We report on a search for Bs0→μ+μ- and B0→μ+μ-
decays using proton-antiproton collision data at √s=1.96
TeV corresponding to 10 fb-1 of integrated luminosity
collected by the CDF II detector at the Fermilab Tevatron
collider. The observed number of B0 candidates is consistent
with background-only expectations and yields an upper limit
on the branching fraction of B(B0→μ+μ-)<4.6×10-9 at 95%
confidence level. We observe an excess of Bs0 candidates.
The probability that the background processes alone could
produce such an excess or larger is 0.94%. The probability
that the combination of background and the expected standard
model rate of Bs0→μ+μ- could produce such an excess or
larger is 6.8%. These data are used to determine a branching
fraction B(Bs0→μ+μ-)=(1.3-0.7+0.9) ×10-8 and provide an
upper limit of B(Bs0→μ +μ-)<3.1×10-8 at 95% confidence
level. © 2013 American Physical Society.},
Doi = {10.1103/PhysRevD.87.072003},
Key = {fds307607}
}
@booklet{Abbott98g,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Goussiou, A and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Dugad, SR and Bantly,
J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram,
I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Astur, R and Biswas,
N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko,
NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross,
A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Valdez, CH and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
C and Vidal, CD and Cummings, MA and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
Y and Dudko, LV and Banerjee, S and Edmunds, D and Ellison, J and Elvira,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein,
D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum,
E and Forden, GE},
Title = {Search for charge-1/3 Third-generation leptoquarks in p¯p
collisions at √s=1.8TeV},
Journal = {Physical Review Letters},
Volume = {81},
Number = {1},
Pages = {38-43},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.38},
Abstract = {We report on a search for charge-1/3 third-generation
leptoquarks (LQ) produced in p¯p collisions at √s=1.8TeV
using the D0 detector at Fermilab. Third-generation
leptoquarks are assumed to be produced in pairs and to decay
to a tau neutrino and a b quark with branching fraction B.
We place upper limits on σ (p¯p→LQ¯LQ)B2 as a function
of the leptoquark mass MLQ. Assuming B=1 we exclude at the
95% confidence level third-generation scalar leptoquarks
with MLQ<94GeV/c2 and third-generation vector leptoquarks
with MLQ<216GeV/c2(MLQ<148GeV/c2) assuming Yang-Mills
(anomalous) coupling. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.81.38},
Key = {Abbott98g}
}
@article{fds357501,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for charged Higgs bosons decaying into a top quark
and a bottom quark at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {6},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2021)145},
Abstract = {A search for charged Higgs bosons decaying into a top quark
and a bottom quark is presented. The data analysed
correspond to 139 fb−1 of proton-proton collisions at s =
13 TeV, recorded with the ATLAS detector at the LHC. The
production of a heavy charged Higgs boson in association
with a top quark and a bottom quark, pp → tbH+ → tbtb,
is explored in the H+ mass range from 200 to 2000 GeV using
final states with jets and one electron or muon. Events are
categorised according to the multiplicity of jets and
b-tagged jets, and multivariate analysis techniques are used
to discriminate between signal and background events. No
significant excess above the background-only hypothesis is
observed and exclusion limits are derived for the production
cross-section times branching ratio of a charged Higgs boson
as a function of its mass; they range from 3.6 pb at 200 GeV
to 0.036 pb at 2000 GeV at 95% confidence level. The results
are interpreted in the hMSSM and Mh125 scenarios. [Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP06(2021)145},
Key = {fds357501}
}
@article{fds356646,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for charged Higgs bosons decaying into top and bottom
quarks at √s=13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {11},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2018)085},
Abstract = {A search for charged Higgs bosons heavier than the top quark
and decaying via H± → tb is presented. The data analysed
corresponds to 36.1 fb−1 of pp collisions at s=13 TeV and
was recorded with the ATLAS detector at the LHC in 2015 and
2016. The production of a charged Higgs boson in association
with a top quark and a bottom quark, pp → tbH±, is
explored in the mass range from mH± = 200 to 2000 GeV using
multi-jet final states with one or two electrons or muons.
Events are categorised according to the multiplicity of jets
and how likely these are to have originated from
hadronisation of a bottom quark. Multivariate techniques are
used to discriminate between signal and background events.
No significant excess above the background-only hypothesis
is observed and exclusion limits are derived for the
production cross-section times branching ratio of a charged
Higgs boson as a function of its mass, which range from 2.9
pb at mH± = 200 GeV to 0.070 pb at mH± = 2000 GeV. The
results are interpreted in two benchmark scenarios of the
Minimal Supersymmetric Standard Model.[Figure not available:
see fulltext.].},
Doi = {10.1007/JHEP11(2018)085},
Key = {fds356646}
}
@article{fds356665,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for charged Higgs bosons decaying via H ±
→ τ ± ντ in the τ+jets and
τ+lepton final states with 36 fb−1 of pp
collision data recorded at √s=13 TeV with the ATLAS
experiment},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {9},
Year = {2018},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2018)139},
Abstract = {Charged Higgs bosons produced either in top-quark decays or
in association with a top-quark, subsequently decaying via
H± → τ±ντ, are searched for in 36.1 fb−1 of
proton-proton collision data at s=13 TeV recorded with the
ATLAS detector. Depending on whether the top-quark produced
together with H± decays hadronically or leptonically, the
search targets τ+jets and τ+lepton final states, in both
cases with a hadronically decaying τ-lepton. No evidence of
a charged Higgs boson is found. For the mass range of mH± =
90–2000 GeV, upper limits at the 95% confidence level are
set on the production cross-section of the charged Higgs
boson times the branching fraction ℬ (H±→ τ±ντ) in
the range 4.2–0.0025 pb. In the mass range 90–160 GeV,
assuming the Standard Model cross-section for tt¯
production, this corresponds to upper limits between 0.25%
and 0.031% for the branching fraction ℬ(t→bH±)×ℬ(H±→τ±ντ).[Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP09(2018)139},
Key = {fds356665}
}
@article{fds313592,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos,
S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold,
H},
Title = {Search for charged Higgs bosons decaying via H±
→ τ±ν in fully hadronic final states using
pp collision data at √s = 8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {3},
Publisher = {Springer Nature},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2015)088},
Abstract = {Abstract: The results of a search for charged Higgs bosons
decaying to a τ lepton and a neutrino, H± → τ±ν, are
presented. The analysis is based on 19.5 fb−1 of
proton-proton collision data at s$$ \sqrt{s} $$ = 8 TeV
collected by the ATLAS experiment at the Large Hadron
Collider. Charged Higgs bosons are searched for in events
consistent with top-quark pair production or in associated
production with a top quark, depending on the considered H±
mass. The final state is characterised by the presence of a
hadronic τ decay, missing transverse momentum, b-tagged
jets, a hadronically decaying W boson, and the absence of
any isolated electrons or muons with high transverse
momenta. The data are consistent with the expected
background from Standard Model processes. A statistical
analysis leads to 95% confidence-level upper limits on the
product of branching ratios ℬ(t → bH±) × ℬ(H± →
τ±ν), between 0.23% and 1.3% for charged Higgs boson
masses in the range 80-160GeV. It also leads to 95%
confidence-level upper limits on the production cross
section times branching ratio, σ(pp → tH± + X) ×
ℬ(H± → τ±ν), between 0.76 pb and 4.5 fb, for
charged Higgs boson masses ranging from 180 GeV to 1000 GeV.
In the context of different scenarios of the Minimal
Supersymmetric Standard Model, these results exclude nearly
all values of tan β above one for charged Higgs boson
masses between 80 GeV and 160 GeV, and exclude a region of
parameter space with high tan β for H± masses between 200
GeV and 250 GeV.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP03(2015)088},
Key = {fds313592}
}
@article{fds307789,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwoo-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio, LB and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G},
Title = {Search for charged Higgs bosons decaying via H±
→ τν in tt̄ events using pp collision data at √s = 7
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {6},
Publisher = {Springer Nature},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP06(2012)039},
Abstract = {The results of a search for charged Higgs bosons are
presented. The analysis is based on 4.6 fb?1 of
proton-proton collision data at √s = 7TeV collected by the
ATLAS experiment at the Large Hadron Collider, using top
quark pair events with a τ lepton in the final state. The
data are consistent with the expected background from
Standard Model processes. Assuming that the branching ratio
of the charged Higgs boson to a τ lepton and a neutrino is
100%, this leads to upper limits on the branching ratio of
top quark decays to a b quark and a charged Higgs boson
between 5% and 1% for charged Higgs boson masses ranging
from 90GeV to 160GeV, respectively. In the context of the
mhmaxscenario of the MSSM, tan β above 12-26, as well as
between 1 and 2-6, can be excluded for charged Higgs boson
masses between 90GeV and 150GeV. Copyright
CERN.},
Doi = {10.1007/JHEP06(2012)039},
Key = {fds307789}
}
@article{fds308103,
Author = {Abulencia, and A, and others},
Title = {Search for charged Higgs bosons from top quark decays in p
anti-p collisions at $\sqrt{s}$ = 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {4},
Pages = {042003},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.042003},
Abstract = {We report the results of a search for a charged Higgs boson
in the decays of top quarks produced in p anti-p collisions
at a center-of-mass energy of 1.96 GeV. We use a data sample
corresponding to an integrated luminosity of 193 pb-1
collected by the upgraded Collider Detector at Fermilab. No
evidence for charged Higgs production is found, allowing 95%
C.L. upper limits to be placed on BR(t --> H+b) for
different charged Higgs decay scenarios. In addition, we
present in the MSSM (m_H+/-, tan B) plane the first
exclusion regions with radiative and Yukawa coupling
corrections.},
Doi = {10.1103/physrevlett.96.042003},
Key = {fds308103}
}
@article{fds308224,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Search for charged higgs bosons in decays of top quark
pairs},
Journal = {Physical Review Letters},
Volume = {82},
Number = {25},
Pages = {4975-4980},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.4975},
Abstract = {We present a search for charged Higgs bosons in decays of
pair-produced top quarks using 109.2 ± 5.8pb-1 of data
recorded from pp collisions at √ s = 1.8 TeV by the D0
detector during 1992-1996 at the Fermilab Tevatron. No
evidence is found for charged Higgs production, and most
parts of the [MH+, tan β] parameter space where the decay t
→ H+ b has a branching fraction close to or larger than
that for t → W+ b are excluded at 95% confidence level.
Assuming mt = 175 GeV and σ(pp → tt) = 5.5 pb, for MH+ =
60 GeV, we exclude tan β < 0.97 and tan β > 40.9. © 1999
The American Physical Society.},
Doi = {10.1103/PhysRevLett.82.4975},
Key = {fds308224}
}
@article{fds307943,
Author = {Aaltonen, T and others},
Title = {Search for Charged Higgs Bosons in Decays of Top Quarks in
pp̅ Collisions at sqrt[s] =1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {10},
Pages = {101803},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.101803},
Abstract = {We report on the first direct search for charged Higgs
bosons decaying into cs̅ in tt̅ events produced by pp̅
collisions at sqrt[s]=1.96 TeV. The search uses a data
sample corresponding to an integrated luminosity of
2.2 fb-1 collected by the CDF II detector at Fermilab
and looks for a resonance in the invariant mass distribution
of two jets in the lepton+jets sample of tt̅ candidates. We
observe no evidence of charged Higgs bosons in top quark
decays. Hence, 95% upper limits on the top quark decay
branching ratio are placed at B(t→H+b)< 0.1 to 0.3 for
charged Higgs boson masses of 60 to 150 GeV/c2 assuming
B(H+→cs̅ )=1.0. The upper limits on B(t→H+b) are also
used as model-independent limits on the decay branching
ratio of top quarks to generic scalar charged bosons beyond
the standard model.},
Doi = {10.1103/physrevlett.103.101803},
Key = {fds307943}
}
@article{fds356773,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Search for charged Higgs bosons in the H± → tb
decay channel in pp collisions at √s = 8 TeV using the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {3},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2016)127},
Abstract = {Charged Higgs bosons heavier than the top quark and decaying
via H± → tb are searched for in proton-proton collisions
measured with the ATLAS experiment at (Formula presented.)
TeV corresponding to an integrated luminosity of 20.3fb−1.
The production of a charged Higgs boson in association with
a top quark, gb → tH±, is explored in the mass range 200
to 600 GeV using multi-jet final states with one electron or
muon. In order to separate the signal from the Standard
Model background, analysis techniques combining several
kinematic variables are employed. An excess of events above
the background-only hypothesis is observed across a wide
mass range, amounting to up to 2.4 standard deviations.
Upper limits are set on the gb → tH± production cross
section times the branching fraction BR(H± → tb).
Additionally, the complementary s-channel production, qq′
→ H±, is investigated through a reinterpretation of W′
→ tb searches in ATLAS. Final states with one electron or
muon are relevant for H± masses from 0.4 to 2.0 TeV,
whereas the all-hadronic final state covers the range 1.5 to
3.0 TeV. In these search channels, no significant excesses
from the predictions of the Standard Model are observed, and
upper limits are placed on the qq′ → H± production
cross section times the branching fraction BR(H± →
tb).},
Doi = {10.1007/JHEP03(2016)127},
Key = {fds356773}
}
@article{fds321101,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for charged Higgs bosons produced in association with
a top quark and decaying via H± → τν using
pp collision data recorded at √s=13 TeV by the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {759},
Pages = {555-574},
Publisher = {Elsevier BV},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2016.06.017},
Abstract = {Charged Higgs bosons produced in association with a single
top quark and decaying via H±→τν are searched for with
the ATLAS experiment at the LHC, using proton–proton
collision data at s=13 TeV corresponding to an integrated
luminosity of 3.2 fb−1. The final state is characterised
by the presence of a hadronic τ decay and missing
transverse momentum, as well as a hadronically decaying top
quark, resulting in the absence of high-transverse-momentum
electrons and muons. The data are found to be consistent
with the expected background from Standard Model processes.
A statistical analysis leads to 95% confidence-level upper
limits on the production cross section times branching
fraction, σ(pp→[b]tH±)×BR(H±→τν), between 1.9 pb
and 15 fb, for charged Higgs boson masses ranging from 200
to 2000 GeV. The exclusion limits for this search surpass
those obtained with the proton–proton collision data
recorded at s=8 TeV.},
Doi = {10.1016/j.physletb.2016.06.017},
Key = {fds321101}
}
@article{fds307617,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Joffe, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
S and Arik, E and Arik, M},
Title = {Search for charged Higgs bosons through the violation of
lepton universality in tt events using pp collision data at
√S=7 TeV with the ATLAS experiment},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {3},
Publisher = {Springer Nature},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP03(2013)076},
Abstract = {In several extensions of the Standard Model, the top quark
can decay into a bottom quark and a light charged Higgs
boson H +, t → bH +, in addition to the Standard Model
decay t → bW. Since W bosons decay to the three lepton
generations equally, while H + maypredominantlydecayinto
τν, charged Higgs bosons can be searched for using the
violation of lepton universality in top quark decays. The
analysis in this paper is based on 4.6 fb-1 of proton-proton
collision data at √s=7 TeV collected by the ATLAS
experiment at the Large Hadron Collider. Signatures
containing leptons (e or μ) and/or a hadronically decaying
τ (τ had) are used. Event yield ratios between e + τ had
and e + μ, as well as between μ + τ had andμ + e, final
states are measured in the data and compared to predictions
from simulations. This ratio-based method reduces the impact
of systematic uncertainties in the analysis. No significant
deviation from the Standard Model predictions is observed.
With the assumption that the branching fraction ℬ (H + →
τν) is 100%, upper limits in the range 3.2%-4.4% can be
placed on the branching fraction ℬ (t → bH +) for
charged Higgs boson masses m H+ in the range 90-140 GeV.
After combination with results from a search for charged
Higgs bosons in t\overline{t} decays using the τ had + jets
final state, upper limits on ℬ (t → bH +) can be set in
the range 0.8%-3.4%, for m H+ in the range 90-160
GeV.[Figure not available: see fulltext.] © 2013 Cern for
the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP03(2013)076},
Key = {fds307617}
}
@article{fds357654,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Zeid, OSA and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz,
VA and Pereira, RA and Arcangeletti, C},
Title = {Search for charged-lepton-flavour violation in Z-boson
decays with the ATLAS detector},
Journal = {Nature Physics},
Volume = {17},
Number = {7},
Pages = {819-825},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1038/s41567-021-01225-z},
Abstract = {Leptons with essentially the same properties apart from
their mass are grouped into three families (or flavours).
The number of leptons of each flavour is conserved in
interactions, but this is not imposed by fundamental
principles. Since the formulation of the standard model of
particle physics, the observation of flavour oscillations
among neutrinos has shown that lepton flavour is not
conserved in neutrino weak interactions. So far, there has
been no experimental evidence that this also occurs in
interactions between charged leptons. Such an observation
would be a sign of undiscovered particles or a yet unknown
type of interaction. Here the ATLAS experiment at the Large
Hadron Collider at CERN reports a constraint on
lepton-flavour-violating effects in weak interactions,
searching for Z-boson decays into a τ lepton and another
lepton of different flavour with opposite electric charge.
The branching fractions for these decays are measured to be
less than 8.1 × 10−6 (eτ) and 9.5 × 10−6 (μτ) at
the 95% confidence level using 139 fb−1 of proton–proton
collision data at a centre-of-mass energy of s=13TeV and
20.3 fb−1 at s=8TeV. These results supersede the limits
from the Large Electron–Positron Collider experiments
conducted more than two decades ago.},
Doi = {10.1038/s41567-021-01225-z},
Key = {fds357654}
}
@article{fds356586,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
JF},
Title = {Search for chargino and neutralino production in final
states with a Higgs boson and missing transverse momentum at
s =13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {100},
Number = {1},
Year = {2019},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.100.012006},
Abstract = {A search is conducted for the electroweak pair production of
a chargino and a neutralino pp→χ1±χ20, where the
chargino decays into the lightest neutralino and a W boson,
χ1±→χ10W±, while the neutralino decays into the
lightest neutralino and a Standard Model-like 125 GeV Higgs
boson, χ20→χ10h. Fully hadronic, semileptonic, diphoton,
and multilepton (electrons, muons) final states with missing
transverse momentum are considered in this search. Higgs
bosons in the final state are identified by either two jets
originating from bottom quarks (h→bb), two photons
(h→γγ), or leptons from the decay modes h→WW, h→ZZ
or h→ττ. The analysis is based on 36.1 fb-1 of s=13 TeV
proton-proton collision data recorded by the ATLAS detector
at the Large Hadron Collider. Observations are consistent
with the Standard Model expectations, and 95%
confidence-level limits of up to 680 GeV in χ1±/χ20 mass
are set in the context of a simplified supersymmetric
model.},
Doi = {10.1103/PhysRevD.100.012006},
Key = {fds356586}
}
@article{fds308048,
Author = {Aaltonen, T and others},
Title = {Search for Chargino-Neutralino Production in $p\overline p$
Collisions at $\sqrt{s}$=1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {19},
Pages = {191806},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.191806},
Abstract = {We present a search for associated production of the
chargino and neutralino supersymmetric particles using up to
1.1 fb-1 of integrated luminosity collected by the CDF II
experiment at the Tevatron p[overline p] collider at
sqrt(s)=1.96 TeV. We analyze events with a large transverse
momentum imbalance and either three charged leptons or two
charged leptons of the same electric charge. The numbers of
observed events are consistent with standard model
expectations. Upper limits on the production cross section
are derived in different theoretical models.},
Doi = {10.1103/physrevlett.99.191806},
Key = {fds308048}
}
@article{fds356650,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A},
Title = {Search for chargino-neutralino production using recursive
jigsaw reconstruction in final states with two or three
charged leptons in proton-proton collisions at s =13 TeV
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {9},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.98.092012},
Abstract = {A search for electroweak production of supersymmetric
particles is performed in two-lepton and three-lepton final
states using recursive jigsaw reconstruction, a technique
that assigns reconstructed objects to the most probable
hemispheres of the decay trees, allowing one to construct
tailored kinematic variables to separate the signal and
background. The search uses data collected in 2015 and 2016
by the ATLAS experiment in s=13 TeV proton-proton collisions
at the CERN Large Hadron Collider corresponding to an
integrated luminosity of 36.1 fb-1. Chargino-neutralino pair
production, with decays via W/Z bosons, is studied in final
states involving leptons and jets and missing transverse
momentum for scenarios with large and intermediate mass
splittings between the parent particle and lightest
supersymmetric particle, as well as for the scenario where
this mass splitting is close to the mass of the Z boson. The
latter case is challenging since the vector bosons are
produced with kinematic properties that are similar to those
in Standard Model processes. Results are found to be
compatible with the Standard Model expectations in the
signal regions targeting large and intermediate mass
splittings, and chargino-neutralino masses up to 600 GeV are
excluded at 95% confidence level for a massless lightest
supersymmetric particle. Excesses of data above the expected
background are found in the signal regions targeting low
mass splittings, and the largest local excess amounts to 3.0
standard deviations.},
Doi = {10.1103/PhysRevD.98.092012},
Key = {fds356650}
}
@article{fds349789,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Search for chargino-neutralino production with mass
splittings near the electroweak scale in three-lepton final
states in s =13 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {101},
Number = {7},
Year = {2020},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.101.072001},
Abstract = {A search for supersymmetry through the pair production of
electroweakinos with mass splittings near the electroweak
scale and decaying via on-shell W and Z bosons is presented
for a three-lepton final state. The analyzed proton-proton
collision data taken at a center-of-mass energy of s=13 TeV
were collected between 2015 and 2018 by the ATLAS experiment
at the Large Hadron Collider, corresponding to an integrated
luminosity of 139 fb-1. A search, emulating the recursive
jigsaw reconstruction technique with easily reproducible
laboratory-frame variables, is performed. The two excesses
observed in the 2015-2016 data recursive jigsaw analysis in
the low-mass three-lepton phase space are reproduced.
Results with the full data set are in agreement with the
Standard Model expectations. They are interpreted to set
exclusion limits at the 95% confidence level on simplified
models of chargino-neutralino pair production for masses up
to 345 GeV.},
Doi = {10.1103/PhysRevD.101.072001},
Key = {fds349789}
}
@article{fds307556,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for charginos nearly mass degenerate with the
lightest neutralino based on a disappearing-track signature
in pp collisions at √(s) = 8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {11},
Pages = {112006-1-112006-23},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.88.112006},
Abstract = {A search is presented for direct chargino production based
on a disappearing-track signature using 20:3 fb-1 of
proton-proton collisions at √s = 8 TeV collected with the
ATLAS experiment at the LHC. In anomaly-mediated
supersymmetry breaking (AMSB) models, the lightest chargino
is nearly mass degenerate with the lightest neutralino and
its lifetime is long enough to be detected in the tracking
detectors by identifying decays that result in tracks with
no associated hits in the outer region of the tracking
system. Some models with supersymmetry also predict
charginos with a significant lifetime. This analysis attains
sensitivity for charginos with a lifetime between 0.1 and 10
ns, and significantly surpasses the reach of the LEP
experiments. No significant excess above the background
expectation is observed for candidate tracks with large
transverse momentum, and constraints on chargino properties
are obtained. In the AMSB scenarios, a chargino mass below
270 GeV is excluded at 95% confidence level.},
Doi = {10.1103/PhysRevD.88.112006},
Key = {fds307556}
}
@article{fds361169,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos,
S},
Title = {Search for chargino–neutralino pair production in final
states with three leptons and missing transverse momentum in
√s=13 TeV pp collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {12},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09749-7},
Abstract = {A search for chargino–neutralino pair production in
three-lepton final states with missing transverse momentum
is presented. The study is based on a dataset of s=13 TeV
pp collisions recorded with the ATLAS detector at the LHC,
corresponding to an integrated luminosity of 139 fb - 1. No
significant excess relative to the Standard Model
predictions is found in data. The results are interpreted in
simplified models of supersymmetry, and statistically
combined with results from a previous ATLAS search for
compressed spectra in two-lepton final states. Various
scenarios for the production and decay of charginos (χ~1±)
and neutralinos (χ~20) are considered. For pure higgsino
χ~1±χ~20 pair-production scenarios, exclusion limits at
95% confidence level are set on χ~20 masses up to 210 GeV.
Limits are also set for pure wino χ~1±χ~20 pair
production, on χ~20 masses up to 640 GeV for decays via
on-shell W and Z bosons, up to 300 GeV for decays via
off-shell W and Z bosons, and up to 190 GeV for decays via
W and Standard Model Higgs bosons.},
Doi = {10.1140/epjc/s10052-021-09749-7},
Key = {fds361169}
}
@article{fds307639,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for contact interactions and large extra dimensions
in dilepton events from pp collisions at √s=7 TeV with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.87.015010},
Abstract = {A search for nonresonant new phenomena, originating from
either contact interactions or large extra spatial
dimensions, has been carried out using events with two
isolated electrons or muons. These events, produced at the
LHC in proton-proton collisions at √s=7 TeV, were recorded
by the ATLAS detector. The data sample, collected throughout
2011, corresponds to an integrated luminosity of 4.9 and 5.0
fb-1 in the e+e - and μ+μ- channels, respectively. No
significant deviations from the Standard Model expectation
are observed. Using a Bayesian approach, 95% confidence
level lower limits ranging from 9.0 to 13.9 TeV are placed
on the energy scale of ℓℓqq contact interactions in the
left-left isoscalar model. Lower limits ranging from 2.4 to
3.9 TeV are also set on the string scale in large extra
dimension models. After combining these limits with results
from a similar search in the diphoton channel, slightly more
stringent limits are obtained.},
Doi = {10.1103/PhysRevD.87.015010},
Key = {fds307639}
}
@article{fds310392,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for contact interactions and large extra dimensions
in the dilepton channel using proton-proton collisions at
[Formula: see text] 8 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {12},
Pages = {3134},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3134-6},
Abstract = {A search is conducted for non-resonant new phenomena in
dielectron and dimuon final states, originating from either
contact interactions or large extra spatial dimensions. The
LHC 2012 proton-proton collision dataset recorded by the
ATLAS detector is used, corresponding to 20 fb[Formula: see
text] at [Formula: see text] = 8 TeV. The dilepton
invariant mass spectrum is a discriminating variable in both
searches, with the contact interaction search additionally
utilizing the dilepton forward-backward asymmetry. No
significant deviations from the Standard Model expectation
are observed. Lower limits are set on the [Formula: see
text] contact interaction scale [Formula: see text] between
15.4 TeV and 26.3 TeV, at the 95 % credibility level. For
large extra spatial dimensions, lower limits are set on the
string scale [Formula: see text] between 3.2 TeV to
5.0 TeV.},
Doi = {10.1140/epjc/s10052-014-3134-6},
Key = {fds310392}
}
@article{fds307731,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov,
A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B},
Title = {Search for contact interactions in dilepton events from pp
collisions at √s=7 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {712},
Number = {1-2},
Pages = {40-58},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.04.026},
Abstract = {This Letter presents a search for contact interactions in
the dielectron and dimuon channels using data from
proton-proton collisions produced by the LHC at s=7 TeV and
recorded by the ATLAS detector. The data sample, collected
in 2011, corresponds to an integrated luminosity of 1.08 and
1.21 fb-1 in the e+e- and μ+μ- channels, respectively. No
significant deviations from the standard model are observed.
Using a Bayesian approach with a prior flat in 1/Λ2, the
following 95% CL lower limits are placed on the energy scale
of ℓℓqq contact interactions: Λ->10.1 TeV
(Λ+>9.4 TeV) in the electron channel and Λ->8.0 TeV
(Λ+>7.0 TeV) in the muon channel for constructive
(destructive) interference in the left-left isoscalar
contact interaction model. Limits are also provided for a
prior flat in 1/Λ4. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.04.026},
Key = {fds307731}
}
@article{fds307866,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
Title = {Search for contact interactions in dimuon events from pp
collisions at √s=7TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {84},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.84.011101},
Abstract = {A search for contact interactions has been performed using
dimuon events recorded with the ATLAS detector in
proton-proton collisions at √s=7TeV. The data sample
corresponds to an integrated luminosity of 42pb-1. No
significant deviation from the standard model is observed in
the dimuon mass spectrum, allowing the following 95% C.L.
limits to be set on the energy scale of contact
interactions: Λ>4.9TeV (4.5 TeV) for constructive
(destructive) interference in the left-left isoscalar
compositeness model. These limits are the most stringent to
date for μμqq contact interactions. 2011 American Physical
Society.},
Doi = {10.1103/PhysRevD.84.011101},
Key = {fds307866}
}
@article{fds356704,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for dark matter and other new phenomena in events
with an energetic jet and large missing transverse momentum
using the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {1},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2018)126},
Abstract = {Results of a search for new phenomena in final states with
an energetic jet and large missing transverse momentum are
reported. The search uses proton-proton collision data
corresponding to an integrated luminosity of 36.1 fb−1 at
a centre-of-mass energy of 13 TeV collected in 2015 and 2016
with the ATLAS detector at the Large Hadron Collider. Events
are required to have at least one jet with a transverse
momentum above 250 GeV and no leptons (e or μ). Several
signal regions are considered with increasing requirements
on the missing transverse momentum above 250 GeV. Good
agreement is observed between the number of events in data
and Standard Model predictions. The results are translated
into exclusion limits in models with pair-produced weakly
interacting dark-matter candidates, large extra spatial
dimensions, and supersymmetric particles in several
compressed scenarios.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP01(2018)126},
Key = {fds356704}
}
@article{fds347505,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Aubry, L and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahrasemani, H and Baines,
JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and Bilbao De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Search for dark matter at [Formula: see text] in final
states containing an energetic photon and large missing
transverse momentum with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {6},
Pages = {393},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4965-8},
Abstract = {Results of a search for physics beyond the Standard Model in
events containing an energetic photon and large missing
transverse momentum with the ATLAS detector at the Large
Hadron Collider are reported. As the number of events
observed in data, corresponding to an integrated luminosity
of 36.1 fb[Formula: see text] of proton-proton collisions
at a centre-of-mass energy of [Formula: see text], is in
agreement with the Standard Model expectations,
model-independent limits are set on the fiducial cross
section for the production of events in this final state.
Exclusion limits are also placed in models where dark-matter
candidates are pair-produced. For dark-matter production via
an axial-vector or a vector mediator in the
<i>s</i>-channel, this search excludes mediator masses below
750-[Formula: see text] for dark-matter candidate masses
below 230-[Formula: see text] at 95% confidence level,
depending on the couplings. In an effective theory of
dark-matter production, the limits restrict the value of the
suppression scale [Formula: see text] to be above [Formula:
see text] at 95% confidence level. A limit is also reported
on the production of a high-mass scalar resonance by
processes beyond the Standard Model, in which the resonance
decays to [Formula: see text] and the <i>Z</i> boson
subsequently decays into neutrinos.},
Doi = {10.1140/epjc/s10052-017-4965-8},
Key = {fds347505}
}
@article{fds307652,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim,
A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for dark matter candidates and large extra dimensions
in events with a jet and missing transverse momentum with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {4},
Publisher = {Springer Nature},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2013)075},
Abstract = {A search for new phenomena in events with a high-energy jet
and large missing transverse momentum is performed using
data from proton-proton collisions at √s=7 TeV with the
ATLAS experiment at the Large Hadron Collider. Four
kinematic regions are explored using a dataset corresponding
to an integrated luminosity of 4.7 fb-1. No excess of events
beyond expectations from Standard Model processes is
observed, and limits are set on large extra dimensions and
the pair production of dark matter particles. © 2013 CERN,
for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP04(2013)075},
Key = {fds307652}
}
@article{fds307640,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates,
RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC},
Title = {Search for dark matter candidates and large extra dimensions
in events with a photon and missing transverse momentum in
pp collision data at sqrt[s]=7 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {110},
Number = {1},
Pages = {011802},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.110.011802},
Abstract = {Results of a search for new phenomena in events with an
energetic photon and large missing transverse momentum in
proton-proton collisions at sqrt[s] = 7 TeV are reported.
Data collected by the ATLAS experiment at the LHC
corresponding to an integrated luminosity of 4.6 fb(-1) are
used. Good agreement is observed between the data and the
standard model predictions. The results are translated into
exclusion limits on models with large extra spatial
dimensions and on pair production of weakly interacting dark
matter candidates.},
Doi = {10.1103/physrevlett.110.011802},
Key = {fds307640}
}
@article{fds356759,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for dark matter in association with a Higgs boson
decaying to b-quarks in pp collisions at √s = 13 TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {765},
Pages = {11-31},
Year = {2017},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2016.11.035},
Abstract = {A search for dark matter pair production in association with
a Higgs boson decaying to a pair of bottom quarks is
presented, using 3.2 fb−1 of pp collisions at a
centre-of-mass energy of 13 TeV collected by the ATLAS
detector at the LHC. The decay of the Higgs boson is
reconstructed as a high-momentum bb¯ system with either a
pair of small-radius jets, or a single large-radius jet with
substructure. The observed data are found to be consistent
with the expected backgrounds. Results are interpreted using
a simplified model with a Z′ gauge boson mediating the
interaction between dark matter and the Standard Model as
well as a two-Higgs-doublet model containing an additional
Z′ boson which decays to a Standard Model Higgs boson and
a new pseudoscalar Higgs boson, the latter decaying into a
pair of dark matter particles.},
Doi = {10.1016/j.physletb.2016.11.035},
Key = {fds356759}
}
@article{fds356716,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Search for dark matter in association with a Higgs boson
decaying to two photons at √s=13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {96},
Number = {11},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.96.112004},
Abstract = {A search for dark matter in association with a Higgs boson
decaying to two photons is presented. This study is based on
data collected with the ATLAS detector, corresponding to an
integrated luminosity of 36.1 fb-1 of proton-proton
collisions at the LHC at a center-of-mass energy of 13 TeV
in 2015 and 2016. No significant excess over the expected
background is observed. Upper limits at 95% confidence level
are set on the visible cross section for beyond the Standard
Model physics processes, and the production cross section
times branching fraction of the Standard Model Higgs boson
decaying into two photons in association with missing
transverse momentum in three different benchmark models.
Limits at 95% confidence level are also set on the observed
signal in two-dimensional mass planes. Additionally, the
results are interpreted in terms of 90% confidence-level
limits on the dark-matter-nucleon scattering cross section,
as a function of the dark-matter particle mass, for a
spin-independent scenario.},
Doi = {10.1103/PhysRevD.96.112004},
Key = {fds356716}
}
@article{fds355555,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R},
Title = {Search for dark matter in association with an energetic
photon in pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {2},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2021)226},
Abstract = {A search for dark matter is conducted in final states
containing a photon and missing transverse momentum in
proton-proton collisions at s = 13 TeV. The data, collected
during 2015–2018 by the ATLAS experiment at the CERN LHC,
correspond to an integrated luminosity of 139 fb−1. No
deviations from the predictions of the Standard Model are
observed and 95% confidence-level upper limits between 2.45
fb and 0.5 fb are set on the visible cross section for
contributions from physics beyond the Standard Model, in
different ranges of the missing transverse momentum. The
results are interpreted as 95% confidence-level limits in
models where weakly interacting dark-matter candidates are
pair-produced via an s-channel axial-vector or vector
mediator. Dark-matter candidates with masses up to 415 (580)
GeV are excluded for axial-vector (vector) mediators, while
the maximum excluded mass of the mediator is 1460 (1470)
GeV. In addition, the results are expressed in terms of 95%
confidence-level limits on the parameters of a model with an
axion-like particle produced in association with a photon,
and are used to constrain the coupling gaZγ of an
axion-like particle to the electroweak gauge bosons. [Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP02(2021)226},
Key = {fds355555}
}
@article{fds356658,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H},
Title = {Search for dark matter in events with a hadronically
decaying vector boson and missing transverse momentum in pp
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {10},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2018)180},
Abstract = {A search for dark matter (DM) particles produced in
association with a hadronically decaying vector boson is
performed using pp collision data at a centre-of-mass energy
of s=13 TeV corresponding to an integrated luminosity of
36.1 fb−1, recorded by the ATLAS detector at the Large
Hadron Collider. This analysis improves on previous searches
for processes with hadronic decays of W and Z bosons in
association with large missing transverse momentum (mono-W/Z
searches) due to the larger dataset and further optimization
of the event selection and signal region definitions. In
addition to the mono-W/Z search, the as yet unexplored
hypothesis of a new vector boson Z′ produced in
association with dark matter is considered (mono-Z′
search). No significant excess over the Standard Model
prediction is observed. The results of the mono-W/Z search
are interpreted in terms of limits on invisible Higgs boson
decays into dark matter particles, constraints on the
parameter space of the simplified vector-mediator model and
generic upper limits on the visible cross sections for
W/Z+DM production. The results of the mono-Z′ search are
shown in the framework of several simplified-model scenarios
involving DM production in association with the Z′
boson.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP10(2018)180},
Key = {fds356658}
}
@article{fds307552,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann,
E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernhard, R and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana,
MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blocki, J and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger,
K and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Buehrer, F and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Caso, C and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau,
B and Chapman, JD and Chapman, JW and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov,
A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Chow,
BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba,
J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron,
ZH},
Title = {Search for dark matter in events with a hadronically
decaying W or Z boson and missing transverse momentum in pp
collisions at √s=8 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {112},
Number = {4},
Pages = {041802},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.112.041802},
Abstract = {A search is presented for dark matter pair production in
association with a W or Z boson in pp collisions
representing 20.3 fb(-1) of integrated luminosity at
√s=8 TeV using data recorded with the ATLAS detector
at the Large Hadron Collider. Events with a hadronic jet
with the jet mass consistent with a W or Z boson, and with
large missing transverse momentum are analyzed. The data are
consistent with the standard model expectations. Limits are
set on the mass scale in effective field theories that
describe the interaction of dark matter and standard model
particles, and on the cross section of Higgs production and
decay to invisible particles. In addition, cross section
limits on the anomalous production of W or Z bosons with
large missing transverse momentum are set in two fiducial
regions.},
Doi = {10.1103/physrevlett.112.041802},
Key = {fds307552}
}
@article{fds310373,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for dark matter in events with a Z boson and missing
transverse momentum in pp collisions at s =8TeV with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.90.012004},
Abstract = {A search is presented for production of dark-matter
particles recoiling against a leptonically decaying Z boson
in 20.3fb-1 of pp collisions at s=8TeV with the ATLAS
detector at the Large Hadron Collider. Events with large
missing transverse momentum and two oppositely charged
electrons or muons consistent with the decay of a Z boson
are analyzed. No excess above the Standard Model prediction
is observed. Limits are set on the mass scale of the contact
interaction as a function of the dark-matter particle mass
using an effective field theory description of the
interaction of dark matter with quarks or with Z bosons.
Limits are also set on the coupling and mediator mass of a
model in which the interaction is mediated by a scalar
particle. © 2014 CERN, for the ATLAS Collaboration.},
Doi = {10.1103/PhysRevD.90.012004},
Key = {fds310373}
}
@article{fds310316,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, M and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson,
M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos, G and Azuma, Y and Baak, MA and Baas,
AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus,
M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov,
SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie,
MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck,
HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner,
FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci,
F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan,
JG},
Title = {Search for dark matter in events with heavy quarks and
missing transverse momentum in [Formula: see text]
collisions with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {2},
Pages = {92},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3306-z},
Abstract = {This article reports on a search for dark matter pair
production in association with bottom or top quarks in
[Formula: see text] of [Formula: see text] collisions
collected at [Formula: see text] TeV by the ATLAS detector
at the LHC. Events with large missing transverse momentum
are selected when produced in association with high-momentum
jets of which one or more are identified as jets containing
[Formula: see text]-quarks. Final states with top quarks are
selected by requiring a high jet multiplicity and in some
cases a single lepton. The data are found to be consistent
with the Standard Model expectations and limits are set on
the mass scale of effective field theories that describe
scalar and tensor interactions between dark matter and
Standard Model particles. Limits on the dark-matter-nucleon
cross-section for spin-independent and spin-dependent
interactions are also provided. These limits are
particularly strong for low-mass dark matter. Using a
simplified model, constraints are set on the mass of dark
matter and of a coloured mediator suitable to explain a
possible signal of annihilating dark matter.},
Doi = {10.1140/epjc/s10052-015-3306-z},
Key = {fds310316}
}
@article{fds313602,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Search for Dark Matter in Events with Missing Transverse
Momentum and a Higgs Boson Decaying to Two Photons in pp
Collisions at sqrt[s]=8 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {115},
Number = {13},
Pages = {131801},
Year = {2015},
Month = {September},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.115.131801},
Abstract = {Results of a search for new phenomena in events with large
missing transverse momentum and a Higgs boson decaying to
two photons are reported. Data from proton-proton collisions
at a center-of-mass energy of 8 TeV and corresponding to an
integrated luminosity of 20.3 fb^{-1} have been collected
with the ATLAS detector at the LHC. The observed data are
well described by the expected standard model backgrounds.
Upper limits on the cross section of events with large
missing transverse momentum and a Higgs boson candidate are
also placed. Exclusion limits are presented for models of
physics beyond the standard model featuring dark-matter
candidates.},
Doi = {10.1103/physrevlett.115.131801},
Key = {fds313602}
}
@article{fds307703,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Bai,
Y and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and d'Errico, M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington, S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Fox, PJ and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic, I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harnik, R and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins,
W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon,
T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr, T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lecompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, C and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys,
J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paus, C and Pellett,
DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for dark matter in events with one jet and missing
transverse energy in pp¯ collisions at √s=1.96
TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {21},
Pages = {211804},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.211804},
Abstract = {We present the results of a search for dark matter
production in the monojet signature. We analyze a sample of
Tevatron pp[over ¯] collisions at √s=1.96 TeV
corresponding to an integrated luminosity of 6.7 fb(-1)
recorded by the CDF II detector. In events with large
missing transverse energy and one energetic jet, we find
good agreement between the standard model prediction and the
observed data. We set 90% confidence level upper limits on
the dark matter production rate. The limits are translated
into bounds on nucleon-dark matter scattering rates which
are competitive with current direct detection bounds on
spin-independent interaction below a dark matter candidate
mass of 5 GeV/c(2), and on spin-dependent interactions up to
masses of 200 GeV/c(2).},
Doi = {10.1103/physrevlett.108.211804},
Key = {fds307703}
}
@article{fds356025,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis,
C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji,
S and Balasubramanian, R and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton,
AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso,
MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
Bylund, O and Besson, N and Bethke, S and Betti, A and Bevan, AJ and Beyer,
J and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla,
JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska,
HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capua, M and Cardarelli,
R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter,
TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Chytka, L and Cieri, D},
Title = {Search for Dark Matter Produced in Association with a Dark
Higgs Boson Decaying into W^{±}W^{∓} or ZZ in Fully
Hadronic Final States from sqrt[s]=13 TeV pp Collisions
Recorded with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {126},
Number = {12},
Pages = {121802},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.126.121802},
Abstract = {Several extensions of the Standard Model predict the
production of dark matter particles at the LHC. An uncharted
signature of dark matter particles produced in association
with VV=W^{±}W^{∓} or ZZ pairs from a decay of a dark
Higgs boson s is searched for using 139 fb^{-1} of pp
collisions recorded by the ATLAS detector at a
center-of-mass energy of 13 TeV. The s→V(qq[over
¯])V(qq[over ¯]) decays are reconstructed with a novel
technique aimed at resolving the dense topology from boosted
VV pairs using jets in the calorimeter and tracking
information. Dark Higgs scenarios with m_{s}>160 GeV
are excluded.},
Doi = {10.1103/physrevlett.126.121802},
Key = {fds356025}
}
@article{fds321071,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for dark matter produced in association with a
hadronically decaying vector boson in pp collisions at
√s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {763},
Pages = {251-268},
Publisher = {Elsevier BV},
Year = {2016},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2016.10.042},
Abstract = {A search is presented for dark matter produced in
association with a hadronically decaying W or Z boson using
3.2 fb−1 of pp collisions at s=13 TeV recorded by the
ATLAS detector at the Large Hadron Collider. Events with a
hadronic jet compatible with a W or Z boson and with large
missing transverse momentum are analysed. The data are
consistent with the Standard Model predictions and are
interpreted in terms of both an effective field theory and a
simplified model containing dark matter.},
Doi = {10.1016/j.physletb.2016.10.042},
Key = {fds321071}
}
@article{fds329964,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark,
MR},
Title = {Search for Dark Matter Produced in Association with a Higgs
Boson Decaying to bb[over ¯] Using 36 fb^{-1} of pp
Collisions at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {119},
Number = {18},
Pages = {181804},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.119.181804},
Abstract = {Several extensions of the standard model predict associated
production of dark-matter particles with a Higgs boson. Such
processes are searched for in final states with missing
transverse momentum and a Higgs boson decaying to a bb[over
¯] pair with the ATLAS detector using 36.1 fb^{-1} of
pp collisions at a center-of-mass energy of 13 TeV at the
LHC. The observed data are in agreement with the standard
model predictions and limits are placed on the associated
production of dark-matter particles and a Higgs
boson.},
Doi = {10.1103/physrevlett.119.181804},
Key = {fds329964}
}
@article{fds315364,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Search for dark matter produced in association with a Higgs
boson decaying to two bottom quarks in pp collisions at s =8
TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {93},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {April},
ISSN = {2470-0010},
url = {http://dx.doi.org/10.1103/PhysRevD.93.072007},
Abstract = {This article reports on a search for dark matter pair
production in association with a Higgs boson decaying to a
pair of bottom quarks, using data from 20.3 fb-1 of pp
collisions at a center-of-mass energy of 8 TeV collected by
the ATLAS detector at the LHC. The decay of the Higgs boson
is reconstructed as a high-momentum bb system with either a
pair of small-radius jets, or a single large-radius jet with
substructure. The observed data are found to be consistent
with the expected Standard Model backgrounds.
Model-independent upper limits are placed on the visible
cross sections for events with a Higgs boson decaying into
bb and large missing transverse momentum with thresholds
ranging from 150 to 400 GeV. Results are interpreted using a
simplified model with a Z′ gauge boson decaying into
different Higgs bosons predicted in a two-Higgs-doublet
model, of which the heavy pseudoscalar Higgs decays into a
pair of dark matter particles. Exclusion limits are also
presented for the mass scales of various effective field
theory operators that describe the interaction between dark
matter particles and the Higgs boson.},
Doi = {10.1103/PhysRevD.93.072007},
Key = {fds315364}
}
@article{fds374253,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Search for dark matter produced in association with a single
top quark and an energetic W boson in √s= 13 TeV pp
collisions with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11582-z},
Abstract = {This paper presents a search for dark matter, χ , using
events with a single top quark and an energetic W boson. The
analysis is based on proton–proton collision data
collected with the ATLAS experiment at s= 13 TeV during LHC
Run 2 (2015–2018), corresponding to an integrated
luminosity of 139 fb - 1 . The search considers final states
with zero or one charged lepton (electron or muon), at least
one b-jet and large missing transverse momentum. In
addition, a result from a previous search considering
two-charged-lepton final states is included in the
interpretation of the results. The data are found to be in
good agreement with the Standard Model predictions and the
results are interpreted in terms of 95% confidence-level
exclusion limits in the context of a class of dark matter
models involving an extended two-Higgs-doublet sector
together with a pseudoscalar mediator particle. The search
is particularly sensitive to on-shell production of the
charged Higgs boson state, H± , arising from the
two-Higgs-doublet mixing, and its semi-invisible decays via
the mediator particle, a: H±→ W±a(→ χχ) . Signal
models with H± masses up to 1.5 TeV and a masses up to 350
GeV are excluded assuming a tan β value of 1. For masses of
a of 150 (250) GeV, tan β values up to 2 are excluded for
H± masses between 200 (400) GeV and 1.5 TeV. Signals with
tan β values between 20 and 30 are excluded for H± masses
between 500 and 800 GeV.},
Doi = {10.1140/epjc/s10052-023-11582-z},
Key = {fds374253}
}
@article{fds359540,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Search for dark matter produced in association with a single
top quark in √s=13 TeV pp collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {10},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09566-y},
Abstract = {This paper presents a search for dark matter in the context
of a two-Higgs-doublet model together with an additional
pseudoscalar mediator, a, which decays into the dark-matter
particles. Processes where the pseudoscalar mediator is
produced in association with a single top quark in the
2HDM+a model are explored for the first time at the LHC.
Several final states which include either one or two charged
leptons (electrons or muons) and a significant amount of
missing transverse momentum are considered. The analysis is
based on proton–proton collision data collected with the
ATLAS experiment at s=13 TeV during LHC Run 2
(2015–2018), corresponding to an integrated luminosity of
139 fb - 1. No significant excess above the Standard Model
predictions is found. The results are expressed as 95%
confidence-level limits on the parameters of the signal
models considered.},
Doi = {10.1140/epjc/s10052-021-09566-y},
Key = {fds359540}
}
@article{fds360568,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S},
Title = {Search for dark matter produced in association with a
Standard Model Higgs boson decaying into b-quarks using the
full Run 2 dataset from the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)209},
Abstract = {The production of dark matter in association with Higgs
bosons is predicted in several extensions of the Standard
Model. An exploration of such scenarios is presented,
considering final states with missing transverse momentum
and b-tagged jets consistent with a Higgs boson. The
analysis uses proton-proton collision data at a
centre-of-mass energy of 13 TeV recorded by the ATLAS
experiment at the LHC during Run 2, amounting to an
integrated luminosity of 139 fb−1. The analysis, when
compared with previous searches, benefits from a larger
dataset, but also has further improvements providing
sensitivity to a wider spectrum of signal scenarios. These
improvements include both an optimised event selection and
advances in the object identification, such as the use of
the likelihood-based significance of the missing transverse
momentum and variable-radius track-jets. No significant
deviation from Standard Model expectations is observed.
Limits are set, at 95% confidence level, in two benchmark
models with two Higgs doublets extended by either a heavy
vector boson Z′ or a pseudoscalar singlet a and which both
provide a dark matter candidate χ. In the case of the
two-Higgs-doublet model with an additional vector boson
Z′, the observed limits extend up to a Z′ mass of 3 TeV
for a mass of 100 GeV for the dark matter candidate. The
two-Higgs-doublet model with a dark matter particle mass of
10 GeV and an additional pseudoscalar a is excluded for
masses of the a up to 520 GeV and 240 GeV for tan β = 1 and
tan β = 10 respectively. Limits on the visible
cross-sections are set and range from to 0.05 fb to 3.26 fb,
depending on the missing transverse momentum and b-quark jet
multiplicity requirements. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP11(2021)209},
Key = {fds360568}
}
@article{fds347464,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Changqiao, C-Q and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati,
L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Search for dark matter produced in association with bottom
or top quarks in s = 13 TeV pp collisions with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {1},
Pages = {18},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5486-1},
Abstract = {A search for weakly interacting massive dark-matter
particles produced in association with bottom or top quarks
is presented. Final states containing third-generation
quarks and missing transverse momentum are considered. The
analysis uses 36.1 fb - 1 of proton-proton collision data
recorded by the ATLAS experiment at s = 13 TeV in 2015 and
2016. No significant excess of events above the estimated
backgrounds is observed. The results are interpreted in the
framework of simplified models of spin-0 dark-matter
mediators. For colour-neutral spin-0 mediators produced in
association with top quarks and decaying into a pair of
dark-matter particles, mediator masses below 50 GeV are
excluded assuming a dark-matter candidate mass of 1 GeV and
unitary couplings. For scalar and pseudoscalar mediators
produced in association with bottom quarks, the search sets
limits on the production cross-section of 300 times the
predicted rate for mediators with masses between 10 and 50
GeV and assuming a dark-matter mass of 1 GeV and unitary
coupling. Constraints on colour-charged scalar simplified
models are also presented. Assuming a dark-matter particle
mass of 35 GeV , mediator particles with mass below 1.1 TeV
are excluded for couplings yielding a dark-matter relic
density consistent with measurements.},
Doi = {10.1140/epjc/s10052-017-5486-1},
Key = {fds347464}
}
@article{fds375226,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha,
PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr,
AJ and Barr, JD and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano
Hurrell, LT and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir,
M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom,
PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir,
O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone,
A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A},
Title = {Search for Dark Photons in Rare Z Boson Decays with the
ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {25},
Pages = {251801},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.131.251801},
Abstract = {A search for events with a dark photon produced in
association with a dark Higgs boson via rare decays of the
standard model Z boson is presented, using 139 fb^{-1}
of sqrt[s]=13 TeV proton-proton collision data recorded
by the ATLAS detector at the Large Hadron Collider. The dark
boson decays into a pair of dark photons, and at least two
of the three dark photons must each decay into a pair of
electrons or muons, resulting in at least two same-flavor
opposite-charge lepton pairs in the final state. The data
are found to be consistent with the background prediction,
and upper limits are set on the dark photon's coupling to
the dark Higgs boson times the kinetic mixing between the
standard model photon and the dark photon, α_{D}ϵ^{2}, in
the dark photon mass range of [5, 40] GeV except for the ϒ
mass window [8.8, 11.1] GeV. This search explores new
parameter space not previously excluded by other
experiments.},
Doi = {10.1103/physrevlett.131.251801},
Key = {fds375226}
}
@article{fds307824,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Aktas, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni,
G},
Title = {Search for decays of stopped, long-lived particles from 7
TeV pp collisions with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {4},
Pages = {1-21},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-1965-6},
Abstract = {New metastable massive particles with electric and colour
charge are features of many theories beyond the Standard
Model. A search is performed for long-lived gluino-based
R-hadrons with the ATLAS detector at the LHC using a data
sample corresponding to an integrated luminosity of 31
pb−1. We search for evidence of particles that have come
to rest in the ATLAS detector and decay at some later time
during the periods in the LHC bunch structure without
proton–proton collisions. No significant deviations from
the expected backgrounds are observed, and a cross-section
limit is set. It can be interpreted as excluding
gluino-based R-hadrons with masses less than 341 GeV at the
95 % C.L., for lifetimes from 10−5to 103seconds and a
neutralino mass of 100 GeV.},
Doi = {10.1140/epjc/s10052-012-1965-6},
Key = {fds307824}
}
@article{fds356581,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Search for diboson resonances in hadronic final states in
139 fb−1 of pp collisions at √s = 13 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {9},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2019)091},
Abstract = {Narrow resonances decaying into W W, W Z or ZZ boson pairs
are searched for in 139 fb−1 of proton-proton collision
data at a centre-of-mass energy of s = 13 TeV recorded with
the ATLAS detector at the Large Hadron Collider from 2015 to
2018. The diboson system is reconstructed using pairs of
high transverse momentum, large-radius jets. These jets are
built from a combination of calorimeter- and tracker-inputs
compatible with the hadronic decay of a boosted W or Z
boson, using jet mass and substructure properties. The
search is performed for diboson resonances with masses
greater than 1.3 TeV. No significant deviations from the
background expectations are observed. Exclusion limits at
the 95% confidence level are set on the production
cross-section times branching ratio into dibosons for
resonances in a range of theories beyond the Standard Model,
with the highest excluded mass of a new gauge boson at 3.8
TeV in the context of mass-degenerate resonances that couple
predominantly to gauge bosons.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP09(2019)091},
Key = {fds356581}
}
@article{fds356697,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for diboson resonances with boson-tagged jets in pp
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {777},
Pages = {91-113},
Year = {2018},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2017.12.011},
Abstract = {Narrow resonances decaying into WW, WZ or ZZ boson pairs are
searched for in 36.7 fb−1 of proton–proton collision
data at a centre-of-mass energy of s=13 TeV recorded with
the ATLAS detector at the Large Hadron Collider in 2015 and
2016. The diboson system is reconstructed using pairs of
large-radius jets with high transverse momentum and tagged
as compatible with the hadronic decay of high-momentum W or
Z bosons, using jet mass and substructure properties. The
search is sensitive to diboson resonances with masses in the
range 1.2–5.0 TeV. No significant excess is observed in
any signal region. Exclusion limits are set at the 95%
confidence level on the production cross section times
branching ratio to dibosons for a range of theories beyond
the Standard Model. Model-dependent lower limits on the mass
of new gauge bosons are set, with the highest limit set at
3.5 TeV in the context of mass-degenerate resonances that
couple predominantly to bosons.},
Doi = {10.1016/j.physletb.2017.12.011},
Key = {fds356697}
}
@article{fds351558,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
Title = {Search for dijet resonances in events with an isolated
charged lepton using √s = 13 TeV proton-proton collision
data collected by the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {6},
Year = {2020},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2020)151},
Abstract = {A search for dijet resonances in events with at least one
isolated charged lepon is performed using 139 fb−1 of s =
13 TeV proton-proton collision data recorded by the ATLAS
detector at the LHC. The dijet invariant-mass (mjj)
distribution constructed from events with at least one
isolated electron or muon is searched in the region 0.22 <
mjj< 6.3 TeV for excesses above a smoothly falling
background from Standard Model processes. Triggering based
on the presence of a lepton in the event reduces limitations
imposed by minimum transverse momentum thresholds for
triggering on jets. This approach allows smaller dijet
invariant masses to be probed than in inclusive dijet
searches, targeting a variety of new-physics models, for
example ones in which a new state is produced in association
with a leptonically decaying W or Z boson. No statistically
significant deviation from the Standard Model background
hypothesis is found. Limits on contributions from generic
Gaussian signals with widths ranging from that determined by
the detector resolution up to 15% of the resonance mass are
obtained for dijet invariant masses ranging from 0.25 TeV to
6 TeV. Limits are set also in the context of several
scenarios beyond the Standard Model, such as the Sequential
Standard Model, a technicolor model, a charged Higgs boson
model and a simplified Dark Matter model. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP06(2020)151},
Key = {fds351558}
}
@article{fds307826,
Author = {Collaboration, AVKWGAEAATLAS},
Title = {Search for dilepton resonances in pp collisions at 7 TeV
with the ATLAS detector},
Journal = {Physical Review Letters},
Volume = {107},
Number = {27},
Pages = {272002},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.107.272002},
Abstract = {This Letter reports on a search for narrow high-mass
resonances decaying into dilepton final states. The data
were recorded by the ATLAS experiment in pp collisions at
√s=7 TeV at the Large Hadron Collider and correspond
to a total integrated luminosity of 1.08 (1.21) fb(-1)
in the e(+)e(-) (μ(+)μ(-)) channel. No statistically
significant excess above the standard model expectation is
observed and upper limits are set at the 95% C.L. on the
cross section times branching fraction of Z' resonances and
Randall-Sundrum gravitons decaying into dileptons as a
function of the resonance mass. A lower mass limit of 1.83
TeV on the sequential standard model Z' boson is set. A
Randall-Sundrum graviton with coupling k/M(Pl)=0.1 is
excluded at 95% C.L. for masses below 1.63
TeV.},
Doi = {10.1103/physrevlett.107.272002},
Key = {fds307826}
}
@article{fds332355,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts,
D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann,
R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV},
Title = {Search for dilepton signatures from minimal low-energy
supergravity in [Formula Presented] collisions at [Formula
Presented] TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {63},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2001},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.63.091102},
Abstract = {We report on a search for supersymmetry using the DØ
detector. The 1994–1996 data sample of [Formula Presented]
TeV [Formula Presented] collisions was analyzed for events
containing two leptons [Formula Presented] or [Formula
Presented] two or more jets, and missing transverse energy.
Assuming the minimal supergravity model, with [Formula
Presented] and [Formula Presented] various thresholds were
employed to optimize the search. No events were found beyond
expectation from the background. We set a lower limit at the
95% C.L. of 255 [Formula Presented] for equal mass squarks
and gluinos for [Formula Presented] and present exclusion
contours in the [Formula Presented] plane for [Formula
Presented]–6. © 2001 The American Physical
Society.},
Doi = {10.1103/PhysRevD.63.091102},
Key = {fds332355}
}
@booklet{Abachi97f,
Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Álvarez, G and Alves,
GA and Amidi, E and Amos, N and Anderson, EW and Aronson, SH and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Bendich, J and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Bischoff, A and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt,
A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty,
D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and De,
K and Del-Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard,
J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahey, S and Fahland, T and Fatyga, M and Fatyga, MK and Featherly, J and Feher, S},
Title = {Search for diphoton events with large missing transverse
energy in pp collisions at = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {78},
Number = {11},
Pages = {2070-2074},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.78.2070},
Abstract = {A search for new physics has been carried out in the channel
pp → γγ + ET, as expected in various supersymmetric
models. We require two photons with transverse energy EγT >
12 GeV and pseudorapidity |ηγ < 1.1. The distribution of
missing transverse energy (ET) is consistent with background
and no events have ET > 25 GeV. We set limits on production
cross sections for selectron, sneutrino, and neutralino
pairs, decaying into photons, which range from about 400 fb
to 1 pb depending on the sparticle masses. A general limit
of 185 fb (95% C.L.) is set on σ(pp → γγET + X), where
eγT > 12 GeV, |ηγ| < 1.1, and ET > 25 GeV. © 1997 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.78.2070},
Key = {Abachi97f}
}
@article{fds307836,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Search for diphoton events with large missing transverse
energy with 36 pb-1 of 7 TeV proton-proton
collision data with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {71},
Number = {10},
Publisher = {Springer Nature},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1744-9},
Abstract = {Making use of 36 pb-1 of proton-proton collision data at
√s = 7 TeV, the ATLAS Collaboration has performed a search
for diphoton events with large missing transverse energy.
Observing no excess of events above the Standard Model
prediction, a 95% Confidence Level (CL) upper limit is set
on the cross section for new physics of σ < 0.38-0.65 pb in
the context of a generalised model of gauge-mediated
supersymmetry breaking (GGM) with a bino-like lightest
neutralino, and of σ < 0.18-0.23 pb in the context of a
specific model with one universal extra dimension (UED). A
95% CL lower limit of 560 GeV, for bino masses above 50 GeV,
is set on the GGM gluino mass, while a lower limit of 1/R >
961 GeV is set on the UED compactification radius R. These
limits provide the most stringent tests of these models to
date.},
Doi = {10.1140/epjc/s10052-011-1744-9},
Key = {fds307836}
}
@article{fds307761,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, SW and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart,
H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
Title = {Search for diphoton events with large missing transverse
momentum in 1 fb -1 of 7 TeV proton-proton
collision data with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {710},
Number = {4-5},
Pages = {519-537},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.02.054},
Abstract = {A search for diphoton events with large missing transverse
momentum has been performed using 1.07 fb -1 of
proton-proton collision data at s=7 TeV recorded with the
ATLAS detector. No excess of events was observed above the
Standard Model prediction and 95% Confidence Level (CL)
upper limits are set on the production cross section for new
physics. The limits depend on each model parameter space and
vary as follows: Λ<(22-129) fb in the context of a
generalised model of gauge-mediated supersymmetry breaking
(GGM) with a bino-like lightest neutralino, σ<(27-91) fb
in the context of a minimal model of gauge-mediated
supersymmetry breaking (SPS8), and σ<(15-27) fb in the
context of a specific model with one universal extra
dimension (UED). A 95% CL lower limit of 805 GeV, for bino
masses above 50 GeV, is set on the GGM gluino mass. Lower
limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking
scale Λ and on the UED compactification scale 1/R,
respectively. These limits provide the most stringent tests
of these models to date. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.02.054},
Key = {fds307761}
}
@article{fds307655,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and A°kesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Search for diphoton events with large missing transverse
momentum in 7 TeV proton-proton collision data with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {718},
Number = {2},
Pages = {411-430},
Publisher = {Elsevier BV},
Year = {2012},
Month = {December},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.10.069},
Abstract = {A search for diphoton events with large missing transverse
momentum has been performed using proton-proton collision
data at s=7 TeV recorded with the ATLAS detector,
corresponding to an integrated luminosity of 4.8 fb-1. No
excess of events was observed above the Standard Model
prediction and model-dependent 95% confidence level
exclusion limits are set. In the context of a generalised
model of gauge-mediated supersymmetry breaking with a
bino-like lightest neutralino of mass above 50 GeV, gluinos
(squarks) below 1.07 TeV (0.87 TeV) are excluded, while a
breaking scale Λ below 196 TeV is excluded for a minimal
model of gauge-mediated supersymmetry breaking. For a
specific model with one universal extra dimension,
compactification scales 1/R<1.40 TeV are excluded. These
limits provide the most stringent tests of these models to
date. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.10.069},
Key = {fds307655}
}
@article{fds307643,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, JF and Arik, E},
Title = {Search for direct chargino production in anomaly-mediated
supersymmetry breaking models based on a disappearing-track
signature in pp collisions at √s=7TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {1},
Publisher = {Springer Nature},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP01(2013)131},
Abstract = {A search for direct chargino production in anomaly-mediated
supersymmetry breaking scenarios is performed in pp
collisions at √s=7TeV using 4.7 fb-1 of data collected
with the ATLAS experiment at the LHC. In these models, the
lightest chargino is predicted to have a lifetime long
enough to be detected in the tracking detectors of collider
experiments. This analysis explores such models by searching
for chargino decays that result in tracks with few
associated hits in the outer region of the tracking system.
The transverse-momentum spectrum of candidate tracks is
found to be consistent with the expectation from the
Standard Model background processes and constraints on
chargino properties are obtained. © 2013 CERN for the
benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP01(2013)131},
Key = {fds307643}
}
@article{fds310320,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Beven, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
Title = {Search for direct pair production of a chargino and a
neutralino decaying to the 125 GeV Higgs boson in [Formula:
see text] TeV [Formula: see text] collisions with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {208},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3408-7},
Abstract = {A search is presented for the direct pair production of a
chargino and a neutralino [Formula: see text], where the
chargino decays to the lightest neutralino and the [Formula:
see text] boson, [Formula: see text], while the neutralino
decays to the lightest neutralino and the 125 GeV Higgs
boson, [Formula: see text]. The final states considered for
the search have large missing transverse momentum, an
isolated electron or muon, and one of the following: either
two jets identified as originating from bottom quarks, or
two photons, or a second electron or muon with the same
electric charge. The analysis is based on 20.3 [Formula:
see text] of [Formula: see text] proton-proton collision
data delivered by the Large Hadron Collider and recorded
with the ATLAS detector. Observations are consistent with
the Standard Model expectations, and limits are set in the
context of a simplified supersymmetric model.},
Doi = {10.1140/epjc/s10052-015-3408-7},
Key = {fds310320}
}
@article{fds310362,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for direct pair production of the top squark in
all-hadronic final states in proton-proton collisions at
√s = 8TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Pages = {1-51},
Publisher = {Springer Nature},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2014)015},
Abstract = {The results of a search for direct pair production of the
scalar partner to the top quark using an integrated
luminosity of 20.1 fb-1 of proton-proton collision data at
yfs = 8 TeV recorded with the ATLAS detector at the LHC are
reported. The top squark is assumed to decay via t → t
χ¯01 or t → b χ1 → bW(*)χ-01, where χ-01 (x1)
denotes the lightest neutralino (chargino) in supersymmetric
models. The search targets a fully-hadronic final state in
events with four or more jets and large missing transverse
momentum. No significant excess over the Standard Model
background prediction is observed, and exclusion limits are
reported in terms of the top squark and neutralino masses
and as a function of the branching fraction of t → t
χ-01. For a branching fraction of 100%, top squark masses
in the range 270-645 GeV are excluded for χ-01 masses below
30GeV. For a branching fraction of 50% to either t → t
χ-01 or t → b χ-01, and assuming the χ¯1 mass to be
twice the χ-01 mass, top squark masses in the range 250-550
GeV are excluded for χ-01 masses below 60
GeV.},
Doi = {10.1007/JHEP09(2014)015},
Key = {fds310362}
}
@article{fds307546,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Search for direct production of charginos and neutralinos in
events with three leptons and missing transverse momentum in
pv s = 8 TeV pp collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {4},
Pages = {1-52},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP04(2014)169},
Abstract = {A search for the direct production of charginos and
neutralinos in final states with three leptons and missing
transverse momentum is presented. The analysis is based on
20.3 fb-1 of vs = 8TeV proton-proton collision data
delivered by the Large Hadron Collider and recorded with the
ATLAS detector. Observations are consistent with the
Standard Model expectations and limits are set in
R-parity-conserving phenomenological Minimal Supersymmetric
Standard Models and in simplified supersymmetric models,
significantly extending previous results. For simplified
supersymmetric models of direct chargino (∼X±1) and
next-to-lightest neutralino (X∼02) production with decays
to lightest neutralino (∼X01) via either all three
generations of sleptons, staus only, gauge bosons, or Higgs
bosons, ∼X± 1 and ∼X02 masses are excluded up to
700GeV, 380GeV, 345GeV, or 148GeV respectively, for a
massless ∼X01.},
Doi = {10.1007/JHEP04(2014)169},
Key = {fds307546}
}
@article{fds307638,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ},
Title = {Search for direct production of charginos and neutralinos in
events with three leptons and missing transverse momentum in
√s=7 TeV pp collisions with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {718},
Number = {3},
Pages = {841-859},
Publisher = {Elsevier BV},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2012.11.039},
Abstract = {A search for the direct production of charginos and
neutralinos in final states with three electrons or muons
and missing transverse momentum is presented. The analysis
is based on 4.7 fb−1 of s=7 TeV proton–proton collision
data delivered by the Large Hadron Collider and recorded
with the ATLAS detector. Observations are consistent with
Standard Model expectations in three signal regions that are
either depleted or enriched in Z-boson decays. Upper limits
at 95% confidence level are set in R-parity conserving
phenomenological minimal supersymmetric models and in
simplified models, significantly extending previous
results.},
Doi = {10.1016/j.physletb.2012.11.039},
Key = {fds307638}
}
@article{fds336987,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Search for direct production of charginos, neutralinos and
sleptons in final states with two leptons and missing
transverse momentum in pp collisions at √s = 8TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {5},
Pages = {1-51},
Publisher = {Springer Nature},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2014)071},
Abstract = {Searches for the electroweak production of charginos,
neutralinos and sleptons in final states characterized by
the presence of two leptons (electrons and muons) and
missing transverse momentum are performed using 20.3 fb-1of
proton-proton collision data at √s = 8TeV recorded with
the ATLAS experiment at the Large Hadron Collider. No
significant excess beyond Standard Model expectations is
observed. Limits are set on the masses of the lightest
chargino, next-to-lightest neutralino and sleptons for
different lightest-neutralino mass hypotheses in simplified
models. Results are also interpreted in various scenarios of
the phenomenological Minimal Supersymmetric Standard
Model.},
Doi = {10.1007/JHEP05(2014)071},
Key = {fds336987}
}
@article{fds352892,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Search for direct production of electroweakinos in final
states with missing transverse momentum and a Higgs boson
decaying into photons in pp collisions at √s = 13 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2020)005},
Abstract = {A search for a chargino-neutralino pair decaying via the 125
GeV Higgs boson into photons is presented. The study is
based on the data collected between 2015 and 2018 with the
ATLAS detector at the LHC, corresponding to an integrated
luminosity of 139 fb−1 of pp collisions at a
centre-of-mass energy of 13 TeV. No significant excess over
the expected background is observed. Upper limits at 95%
confidence level for a massless χ˜10 are set on several
electroweakino production cross-sections and the visible
cross-section for beyond the Standard Model processes. In
the context of simplified supersymmetric models, 95%
confidence-level limits of up to 310 GeV in
m(χ˜1±/χ˜20), where m(χ˜10) = 0.5 GeV, are set.
Limits at 95% confidence level are also set on the
χ˜1±χ˜20 cross-section in the mass plane of
m(χ˜1±/χ˜20) and m(χ˜10), and on scenarios with
gravitino as the lightest supersymmetric particle. Upper
limits at the 95% confidence-level are set on the higgsino
production cross-section. Higgsino masses below 380 GeV are
excluded for the case of the higgsino fully decaying into a
Higgs boson and a gravitino. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2020)005},
Key = {fds352892}
}
@article{fds351473,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abulaiti, Y and Abreu, H and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Bella, LA and Arabidze, G},
Title = {Search for direct production of electroweakinos in final
states with one lepton, missing transverse momentum and a
Higgs boson decaying into two b-jets in pp collisions at
√s=13 TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {8},
Publisher = {Springer Science and Business Media LLC},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-8050-3},
Abstract = {The results of a search for electroweakino pair production
pp→χ~1±χ~20 in which the chargino (χ~1±) decays into
a W boson and the lightest neutralino (χ~10), while the
heavier neutralino (χ~20) decays into the Standard Model
125 GeV Higgs boson and a second χ~10 are presented. The
signal selection requires a pair of b-tagged jets consistent
with those from a Higgs boson decay, and either an electron
or a muon from the W boson decay, together with missing
transverse momentum from the corresponding neutrino and the
stable neutralinos. The analysis is based on data
corresponding to 139 fb - 1 of s=13 TeV pp collisions
provided by the Large Hadron Collider and recorded by the
ATLAS detector. No statistically significant evidence of an
excess of events above the Standard Model expectation is
found. Limits are set on the direct production of the
electroweakinos in simplified models, assuming pure wino
cross-sections. Masses of χ~1±/χ~20 up to 740 GeV are
excluded at 95% confidence level for a massless
χ~10.},
Doi = {10.1140/epjc/s10052-020-8050-3},
Key = {fds351473}
}
@article{fds307637,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, M-L and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, R and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansi, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Da Costa and JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Be, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, E and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki,
J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, JJ and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de
Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Buanes, T and Buat, QQ and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov,
O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans, RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, JJ and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez,
AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi,
G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Io, MAC and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and El
Moursli, RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, R and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C},
Title = {Search for direct slepton and gaugino production in final
states with two leptons and missing transverse momentum with
the ATLAS detector in pp collisions at √s=7
TeV},
Journal = {PHYSICS LETTERS B},
Volume = {718},
Number = {3},
Pages = {879-901},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2012.11.058},
Abstract = {A search for the electroweak pair production of charged
sleptons and weak gauginos decaying into final states with
two leptons is performed using 4.7 fb-1 of proton-proton
collision data at s=7 TeV recorded with the ATLAS experiment
at the Large Hadron Collider. No significant excesses are
observed with respect to the prediction from Standard Model
processes. In the scenario of direct slepton production, if
the sleptons decay directly into the lightest neutralino,
left-handed slepton masses between 85 and 195 GeV are
excluded at 95% confidence level for a 20 GeV neutralino.
Chargino masses between 110 and 340 GeV are excluded in the
scenario of direct production of wino-like chargino pairs
decaying into the lightest neutralino via an intermediate
on-shell charged slepton for a 10 GeV neutralino. The
results are also interpreted in the framework of the
phenomenological minimal supersymmetric Standard Model. ©
2012 CERN.},
Doi = {10.1016/j.physletb.2012.11.058},
Key = {fds307637}
}
@article{fds349435,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Search for direct stau production in events with two
hadronic τ-leptons in s =13 TeV pp collisions with the
ATLAS detector},
Journal = {Physical Review D},
Volume = {101},
Number = {3},
Year = {2020},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.101.032009},
Abstract = {A search for the direct production of the supersymmetric
partners of τ-leptons (staus) in final states with two
hadronically decaying τ-leptons is presented. The analysis
uses a dataset of pp collisions corresponding to an
integrated luminosity of 139 fb-1, recorded with the ATLAS
detector at the Large Hadron Collider at a center-of-mass
energy of 13 TeV. No significant deviation from the expected
Standard Model background is observed. Limits are derived in
scenarios of direct production of stau pairs with each stau
decaying into the stable lightest neutralino and one
τ-lepton in simplified models where the two stau mass
eigenstates are degenerate. Stau masses from 120 GeV to 390
GeV are excluded at 95% confidence level for a massless
lightest neutralino.},
Doi = {10.1103/PhysRevD.101.032009},
Key = {fds349435}
}
@article{fds307575,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou-Zeid, OS and Abramowicz, H and Abreu, H and Kuday, S and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Chekanov, S and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Ammosov, VV and Dos Santos,
SPA and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Anulli,
F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Search for direct third-generation squark pair production in
final states with missing transverse momentum and two b-jets
in √s = 8 TeV pp collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {10},
Publisher = {Springer Nature},
Year = {2013},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP10(2013)189},
Abstract = {The results of a search for pair production of
supersymmetric partners of the Standard Model
third-generation quarks are reported. This search uses 20.1
fb−1 of pp collisions at √s = 8TeV collected by the
ATLAS experiment at the Large Hadron Collider. The lightest
bottom and top squarks (b1 and t1 respectively) are searched
for in a final state with large missing transverse momentum
and two jets identified as originating from b-quarks. No
excess of events above the expected level of Standard Model
background is found. The results are used to set upper
limits on the visible cross section for processes beyond the
Standard Model. Exclusion limits at the 95% confidence level
on the masses of the third-generation squarks are derived in
phenomenological supersymmetric R-parityconserving models in
which either the bottom or the top squark is the lightest
squark. The b1 is assumed to decay via b1 → bχ01 and the
t1 via t1 → bχ±1, with undetectable products of the
subsequent decay of the χ±1 due to the small mass
splitting between the χ±1 and the χ01.},
Doi = {10.1007/JHEP10(2013)189},
Key = {fds307575}
}
@article{fds356743,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for direct top squark pair production in events with
a Higgs or Z boson, and missing transverse momentum in
√s=13 TeV pp collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {8},
Year = {2017},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2017)006},
Abstract = {A search for direct top squark pair production resulting in
events with either a same-flavour opposite-sign dilepton
pair with invariant mass compatible with a Z boson or a pair
of jets compatible with a Standard Model (SM) Higgs boson
(h) is presented. Requirements on the missing transverse
momentum, together with additional selections on leptons,
jets, jets identified as originating from b-quarks are
imposed to target the other decay products of the top squark
pair. The analysis is performed using proton-proton
collision data at s=13 TeV collected with the ATLAS detector
at the LHC in 2015–2016, corresponding to an integrated
luminosity of 36.1 fb−1. No excess is observed in the data
with respect to the SM predictions. The results are
interpreted in two sets of models. In the first set, direct
production of pairs of lighter top squarks (t˜ 1) with long
decay chains involving Z or Higgs bosons is considered. The
second set includes direct pair production of the heavier
top squark pairs (t˜ 2) decaying via t˜ 2→ Zt˜ 1 or t˜
2→ ht˜ 1. The results exclude at 95% confidence level t˜
2 and t˜ 1 masses up to about 800 GeV, extending the
exclusion region of supersymmetric parameter space covered
by previous LHC searches.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP08(2017)006},
Key = {fds356743}
}
@article{fds310395,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai,
Y and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas, E and Banerjee, S and Banfi, D and Bangert, A and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Guimarães da Costa and JB and Bartoldus, R and Barton,
AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black,
CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm,
J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Toro, RC and Camarda, S and Cameron, D and Caminada, LM and Armadans, RC and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Barajas, CAC and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli,
R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Christidi, IA and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens,
JC},
Title = {Search for direct top squark pair production in events with
a [Formula: see text] boson, [Formula: see text]-jets and
missing transverse momentum in [Formula: see text] TeV
[Formula: see text] collisions with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {6},
Pages = {2883},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2883-6},
Abstract = {A search is presented for direct top squark pair production
using events with at least two leptons including a
same-flavour opposite-sign pair with invariant mass
consistent with the [Formula: see text] boson mass, jets
tagged as originating from [Formula: see text]-quarks and
missing transverse momentum. The analysis is performed with
proton-proton collision data at [Formula: see text]
collected with the ATLAS detector at the LHC in 2012
corresponding to an integrated luminosity of
20.3 fb[Formula: see text]. No excess beyond the Standard
Model expectation is observed. Interpretations of the
results are provided in models based on the direct pair
production of the heavier top squark state ([Formula: see
text]) followed by the decay to the lighter top squark state
([Formula: see text]) via [Formula: see text], and for
[Formula: see text] pair production in natural
gauge-mediated supersymmetry breaking scenarios where the
neutralino ([Formula: see text]) is the next-to-lightest
supersymmetric particle and decays producing a [Formula: see
text] boson and a gravitino ([Formula: see text]) via the
[Formula: see text] process.},
Doi = {10.1140/epjc/s10052-014-2883-6},
Key = {fds310395}
}
@article{fds307667,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, AD and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia,
A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker,
C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for direct top squark pair production in final states
with one isolated lepton, jets, and missing transverse
momentum in sqrt[s] = 7 TeV pp collisions using 4.7 fb(-10
of ATLAS data.},
Journal = {Physical review letters},
Volume = {109},
Number = {21},
Pages = {211803},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.109.211803},
Abstract = {A search is presented for direct top squark pair production
in final states with one isolated electron or muon, jets,
and missing transverse momentum in proton-proton collisions
at sqrt[s] = 7 TeV. The measurement is based on 4.7 fb(-1)
of data collected with the ATLAS detector at the LHC. Each
top squark is assumed to decay to a top quark and the
lightest supersymmetric particle (LSP). The data are found
to be consistent with standard model expectations. Top
squark masses between 230 GeV and 440 GeV are excluded with
95% confidence for massless LSPs, and top squark masses
around 400 GeV are excluded for LSP masses up to 125
GeV.},
Doi = {10.1103/physrevlett.109.211803},
Key = {fds307667}
}
@article{fds348507,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and AlconadaVerzini, MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and AlvarezGonzalez, B and ÁlvarezPiqueras, D and Alviggi, MG and Amadio, BT and AmaralCoutinho, Y and Amelung, C and Amidei, D and AmorDosSantos, SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and AperioBella, L and Arabidze, G and Arai, Y and Araque, JP and AraujoFerraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic,
M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin,
DL and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock,
I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt,
BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini,
I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Search for direct top squark pair production in final states
with two leptons in s = 13 TeV pp collisions with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {12},
Pages = {898},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5445-x},
Abstract = {The results of a search for direct pair production of top
squarks in events with two opposite-charge leptons
(electrons or muons) are reported, using 36.1 fb - 1 of
integrated luminosity from proton-proton collisions at s =
13 TeV collected by the ATLAS detector at the Large Hadron
Collider. To cover a range of mass differences between the
top squark t ~ and lighter supersymmetric particles, four
possible decay modes of the top squark are targeted with
dedicated selections: the decay t ~ → b χ ~ 1 ± into a
<i>b</i>-quark and the lightest chargino with χ ~ 1 ± →
W χ ~ 1 0 , the decay t ~ → t χ ~ 1 0 into an on-shell
top quark and the lightest neutralino, the three-body decay
t ~ → b W χ ~ 1 0 and the four-body decay t ~ → b ℓ
ν χ ~ 1 0 . No significant excess of events is observed
above the Standard Model background for any selection, and
limits on top squarks are set as a function of the t ~ and
χ ~ 1 0 masses. The results exclude at 95% confidence level
t ~ masses up to about 720 GeV, extending the exclusion
region of supersymmetric parameter space covered by previous
searches.},
Doi = {10.1140/epjc/s10052-017-5445-x},
Key = {fds348507}
}
@article{fds347517,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot,
J},
Title = {Search for direct top squark pair production in final states
with two tau leptons in pp collisions at [Formula:
see text] TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {81},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-3897-z},
Abstract = {A search for direct pair production of the supersymmetric
partner of the top quark, decaying via a scalar tau to a
nearly massless gravitino, has been performed using
20 fb[Formula: see text] of proton-proton collision data at
[Formula: see text]. The data were collected by the ATLAS
experiment at the LHC in 2012. Top squark candidates are
searched for in events with either two hadronically decaying
tau leptons, one hadronically decaying tau and one light
lepton, or two light leptons. No significant excess over the
Standard Model expectation is found. Exclusion limits at
[Formula: see text] confidence level are set as a function
of the top squark and scalar tau masses. Depending on the
scalar tau mass, ranging from the [Formula: see text] LEP
limit to the top squark mass, lower limits between 490 and
[Formula: see text] are placed on the top squark mass within
the model considered.},
Doi = {10.1140/epjc/s10052-016-3897-z},
Key = {fds347517}
}
@article{fds310375,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Ammosov, VV and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for direct top-squark pair production in final states
with two leptons in pp collisions at √s = 8 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {6},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2014)124},
Abstract = {A search is presented for direct top-squark pair production
in final states with two leptons (electrons or muons) of
opposite charge using 20.3 fb -1 of pp collision data at
√s = 8 TeV, collected by the ATLAS experiment at the Large
Hadron Collider in 2012. No excess over the Standard Model
expectation is found. The results are interpreted under the
separate assumptions (i) that the top squark decays to a
b-quark in addition to an on-shell chargino whose decay
occurs via a real or virtual W boson, or (ii) that the top
squark decays to a t-quark and the lightest neutralino. A
top squark with a mass between 150 GeV and 445 GeV decaying
to a b-quark and an on-shell chargino is excluded at 95%
confidence level for a top squark mass equal to the chargino
mass plus 10 GeV, in the case of a 1 GeV lightest
neutralino. Top squarks with masses between 215 (90) GeV and
530 (170) GeV decaying to an on-shell (off-shell) t-quark
and a neutralino are excluded at 95% confidence level for a
1 GeV neutralino. [Figure not available: see fulltext.] ©
2014 The Author(s).},
Doi = {10.1007/JHEP06(2014)124},
Key = {fds310375}
}
@article{fds366278,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Austrup, VA and Avolio,
G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey,
AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker,
PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian,
R and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos,
P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Basson,
CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer,
F and Bechtle, P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
Kuutmann, E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer,
J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
Bylund, O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman,
M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich,
C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio
Sola, JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler,
S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski,
JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, Y and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casado,
MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia,
L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli,
F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan,
J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chau, CC and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski,
JJ and Cieri, D and Ciesla, KM and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clawson, SE and Clement, C and Clissa, L and Coadou, Y and Cobal, M and Coccaro, A},
Title = {Search for Displaced Leptons in sqrt[s]=13 TeV pp
Collisions with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {127},
Number = {5},
Pages = {051802},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.127.051802},
Abstract = {A search for charged leptons with large impact parameters
using 139 fb^{-1} of sqrt[s]=13 TeV pp collision
data from the ATLAS detector at the LHC is presented,
addressing a long-standing gap in coverage of possible new
physics signatures. Results are consistent with the
background prediction. This search provides unique
sensitivity to long-lived scalar supersymmetric lepton
partners (sleptons). For lifetimes of 0.1 ns, selectron,
smuon, and stau masses up to 720, 680, and 340 GeV,
respectively, are excluded at 95% confidence level,
drastically improving on the previous best limits from
LEP.},
Doi = {10.1103/physrevlett.127.051802},
Key = {fds366278}
}
@article{fds310401,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Search for displaced muonic lepton jets from light Higgs
boson decay in proton–proton collisions at √s = 7 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {721},
Number = {1-3},
Pages = {32-50},
Publisher = {Elsevier BV},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2013.02.058},
Abstract = {A search is performed for collimated muon pairs displaced
from the primary vertex produced in the decay of long-lived
neutral particles in proton–proton collisions at s=7 TeV
centre-of-mass energy, with the ATLAS detector at the LHC.
In a 1.9 fb−1event sample collected during 2011, the
observed data are consistent with the Standard Model
background expectations. Limits on the product of the
production cross section and the branching ratio of a Higgs
boson decaying to hidden-sector neutral long-lived particles
are derived as a function of the particlesʼ mean
lifetime.},
Doi = {10.1016/j.physletb.2013.02.058},
Key = {fds310401}
}
@article{fds373543,
Author = {Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben,
M and Bouquet, R and Marchiori, G and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Wang, R and Zhang, J and Berlendis, S and Cheu, E and Cui,
Z and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK and Unal, M and Webb, AF and Huseynov, N and Agaras, MN and Bosman, M and Casado,
MP},
Title = {Search for displaced photons produced in exotic decays of
the Higgs boson using 13 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032016},
Abstract = {A search is performed for delayed and nonpointing photons
originating from the displaced decay of a neutral long-lived
particle (LLP). The analysis uses the full run 2 dataset of
proton-proton collisions delivered by the LHC at a
center-of-mass energy of Formula Presented between 2015 and
2018 and recorded by the ATLAS detector, corresponding to an
integrated luminosity of Formula Presented. The capabilities
of the ATLAS electromagnetic calorimeter are exploited to
precisely measure the arrival times and trajectories of
photons. The results are interpreted in a scenario where the
LLPs are pair produced in exotic decays of the 125 GeV Higgs
boson, and each LLP subsequently decays into a photon and a
particle that escapes direct detection, giving rise to
missing transverse momentum. No significant excess is
observed above the expectation due to Standard Model
background processes. The results are used to set upper
limits on the branching ratio of the exotic decay of the
Higgs boson. A model-independent limit is also set on the
production of photons with large values of displacement and
time delay.},
Doi = {10.1103/PhysRevD.108.032016},
Key = {fds373543}
}
@article{fds307759,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Search for displaced vertices arising from decays of new
heavy particles in 7 TeV pp collisions at
ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {707},
Number = {5},
Pages = {478-496},
Publisher = {Elsevier BV},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2011.12.057},
Abstract = {We present the results of a search for new, heavy particles
that decay at a significant distance from their production
point into a final state containing charged hadrons in
association with a high-momentum muon. The search is
conducted in a pp-collision data sample with a
center-of-mass energy of 7 TeV and an integrated luminosity
of 33 pb-1 collected in 2010 by the ATLAS detector operating
at the Large Hadron Collider. Production of such particles
is expected in various scenarios of physics beyond the
standard model. We observe no signal and place limits on the
production cross-section of supersymmetric particles in an
R-parity-violating scenario as a function of the neutralino
lifetime. Limits are presented for different squark and
neutralino masses, enabling extension of the limits to a
variety of other models. © 2011 CERN.},
Doi = {10.1016/j.physletb.2011.12.057},
Key = {fds307759}
}
@article{fds356539,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R},
Title = {Search for displaced vertices of oppositely charged leptons
from decays of long-lived particles in pp collisions at s=13
TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {801},
Year = {2020},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2019.135114},
Abstract = {A search for long-lived particles decaying into an
oppositely charged lepton pair, μμ, ee, or eμ, is
presented using 32.8fb−1 of pp collision data collected at
s=13 TeV by the ATLAS detector at the LHC. Candidate leptons
are required to form a vertex, within the inner tracking
volume of ATLAS, displaced from the primary pp interaction
region. No lepton pairs with an invariant mass greater than
12 GeV are observed, consistent with the background
expectations derived from data. The detection efficiencies
for generic resonances with lifetimes (cτ) of 100–1000 mm
decaying into a dilepton pair with masses between 0.1–1.0
TeV are presented as a function of pT and decay radius of
the resonances to allow the extraction of upper limits on
the cross sections for theoretical models. The result is
also interpreted in a supersymmetric model in which the
lightest neutralino, produced via squark–antisquark
production, decays into ℓ+ℓ′−ν (ℓ,ℓ′=e, μ)
with a finite lifetime due to the presence of R-parity
violating couplings. Cross-section limits are presented for
specific squark and neutralino masses. For a 700 GeV squark,
neutralinos with masses of 50–500 GeV and mean proper
lifetimes corresponding to cτ values between 1 mm to 6 m
are excluded. For a 1.6 TeV squark, cτ values between 3 mm
to 1 m are excluded for 1.3 TeV neutralinos.},
Doi = {10.1016/j.physletb.2019.135114},
Key = {fds356539}
}
@article{fds357645,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
S},
Title = {Search for doubly and singly charged Higgs bosons decaying
into vector bosons in multi-lepton final states with the
ATLAS detector using proton-proton collisions at √s = 13
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {6},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2021)146},
Abstract = {A search for charged Higgs bosons decaying into W±W± or
W±Z bosons is performed, involving experimental signatures
with two leptons of the same charge, or three or four
leptons with a variety of charge combinations, missing
transverse momentum and jets. A data sample of proton-proton
collisions at a centre-of-mass energy of 13 TeV recorded
with the ATLAS detector at the Large Hadron Collider between
2015 and 2018 is used. The data correspond to a total
integrated luminosity of 139 fb−1. The search is guided by
a type-II seesaw model that extends the scalar sector of the
Standard Model with a scalar triplet, leading to a
phenomenology that includes doubly and singly charged Higgs
bosons. Two scenarios are explored, corresponding to the
pair production of doubly charged H±± bosons, or the
associated production of a doubly charged H±± boson and a
singly charged H± boson. No significant deviations from the
Standard Model predictions are observed. H±± bosons are
excluded at 95% confidence level up to 350 GeV and 230 GeV
for the pair and associated production modes, respectively.
[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP06(2021)146},
Key = {fds357645}
}
@article{fds308161,
Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahmed, SN and Ahn,
SH and Alexeev, GD and Alkhazov, G and Alton, A and Alverson, G and Alves,
GA and Anderson, S and Andrieu, B and Arnoud, Y and Askew, A and Asman, B and Autermann, C and Avila, C and Babukhadia, L and Bacon, TC and Baden, A and Baffioni, S and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer, P and Barnes, C and Barreto, J and Bartlett,
JF and Bassler, U and Bauer, D and Bean, A and Beauceron, S and Beaudette,
F and Begel, M and Beri, SB and Bernardi, G and Bertram, I and Besançon,
M and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Binder, M and Bischoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Bloch, D and Blumenschein, U and Boehnlein, A and Bolton, TA and Bonamy, P and Borcherding, F and Borissov, G and Bos, K and Bose, T and Boswell, C and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burdin, S and Burnett,
TH and Busato, E and Butler, JM and Bystricky, J and Canelli, F and Carvalho, W and Casey, BCK and Casey, D and Cason, NM and Castilla-Valdez, H and Chakrabarti, S and Chakraborty, D and Chan,
KM and Chandra, A and Chapin, D and Charles, F and Cheu, E and Chevalier,
L and Cho, DK and Choi, S and Chopra, S and Christiansen, T and Christofek,
L and Claes, D and Clark, AR and Clément, C and Coadou, Y and Colling, DJ and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Corcoran, M and Coss, J and Cothenet, A and Cousinou, M-C and Crépé-Renaudin, S and Cristetiu, M and Cummings, MAC and Cutts, D and da Motta, H and Davies,
B and Davies, G and Davis, GA and De, K and de Jong, P and de Jong, SJ and De
La Cruz-Burelo and E and De Oliveira Martins and C and Dean, S and Del
Signore, K and Déliot, F and Delsart, PA and Demarteau, M and Demina,
R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doidge, M and Dong, H and Doulas, S and Duflot, L and Dugad, SR and Duperrin, A and Dyer, J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Eltzroth,
JT and Elvira, VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Fein, D and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisk, HE and Fleuret, F and Fortner, M and Fox, H and Freeman, W and Fu, S and Fuess, S and Galea, CF and Gallas, E and Galyaev,
E and Gao, M and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gelé, D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Geurkov, G and Ginther, G and Goldmann, K and Golling,
T and Gómez, B and Gounder, K and Goussiou, A and Graham, G and Grannis,
PD and Greder, S and Green, JA and Greenlee, H and Greenwood, ZD and Gregores, EM and Grinstein, S and Grivaz, J-F and Groer, L and Grünendahl, S and Grünewald, MW and Gu, W and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley, NJ and Haggerty,
H and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki,
K and Hanlet, P and Harder, K and Hauptman, JM and Hauser, R and Hays, C and Hays, J and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper, R and Hou, S and Hu, Y and Huang, J and Huang, Y and Iashvili, I and Illingworth,
R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs,
K and Jenkins, A and Jesik, R and Jiang, Y and Johns, K and Johnson, M and Johnson, P and Jonckheere, A and Jonsson, P and Jöstlein, H and Juste,
A and Kado, MM and Käfer, D and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Ke, Z and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov, A and Kharchilava, A and Kharzheev, YM and Kim, KH and Klima, B and Klute, M and Kohli, JM and Kopal, M and Korablev, V and Kotcher, J and Kothari, B and Kotwal, AV and Koubarovsky, A and Kouchner, A and Kouznetsov, O and Kozelov, AV and Kozminski, J and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kurca, T and Kuznetsov, VE and Lager, S and Lahrichi, N and Landsberg, G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee, SW and Lee, WM and Leflat, A and Leggett, C and Lehner,
F and Leonidopoulos, C and Lewis, P and Li, J and Li, QZ and Li, X and Lima,
JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lobo, L and Lobodenko, A and Lokajicek, M and Lounis, A and Lu, J and Lubatti, HJ and Lucotte, A and Lueking, L and Luo, C and Lynker, M and Lyon, AL and Maciel,
AKA and Madaras, RJ and Magnan, A-M and Maity, M and Mal, PK and Malik, S and Malyshev, VL and Manankov, V and Mao, HS and Maravin, Y and Marshall, T and Martens, M and Martin, MI and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and McMahon, T and Meder, D and Melanson,
HL and Melnitchouk, A and Meng, X and Merkin, M and Merritt, KW and Meyer,
A and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mitrevski, J and Mokhov, N and Molina, J and Mondal, NK and Montgomery,
HE and Moore, RW and Mostafa, M and Muanza, GS and Mulders, M and Mutaf,
YD and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann,
NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding,
C and Nomerotski, A and Novaes, SF and Nunnemann, T and Nurse, E and O'Dell, V and O'Neil, DC and Oguri, V and Oliveira, N and Olivier, B and Oshima, N and Otero y Garzón and GJ and Padley, P and Papageorgiou, K and Parashar, N and Park, J and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Peters, O and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Podesta-Lerma,
PLM and Podstavkov, VM and Pope, BG and Popkov, E and Prado da Silva,
WL and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Quadt, A and Quinn, B and Rani, KJ and Rapidis, PA and Ratoff, PN and Reay,
NW and Renardy, J-F and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Royon, C and Rubinov, P and Ruchti, R and Sabirov, BM and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro, A and Savage, G and Sawyer, L and Scanlon, T and Schamberger, RD and Schellman, H and Schieferdecker, P and Schmitt, C and Schukin, A and Schwartzman, A and Schwienhorst, R and Sengupta, S and Shabalina, E and Shary, V and Shephard, WD and Shpakov, D and Sidwell, RA and Simak, V and Sirotenko,
V and Skow, D and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Song, Y and Sonnenschein, L and Sopczak, A and Sorín, V and Sosebee, M and Soustruznik, K and Souza, M and Stanton, NR and Stark, J and Steele, J and Steinbrück, G and Stevenson, K and Stolin, V and Stone, A and Stoyanova, DA and Strandberg, J and Strang, MA and Strauss, M and Ströhmer, R and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Tamburello, P and Taylor, W and Telford, P and Temple, J and Tentindo-Repond, S and Thomas, E and Thooris, B and Tomoto, M and Toole,
T},
Title = {Search for doubly charged higgs boson pair production in the
decay to mu(+)mu(+)mu(-)mu(-) in pp collisions at
sqrt[s]=1.96 TeV.},
Journal = {Physical review letters},
Volume = {93},
Number = {14},
Pages = {141801},
Year = {2004},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.93.141801},
Abstract = {A search for pair production of doubly charged Higgs bosons
in the process pp -->H(++)H(--) -->mu(+)mu(+)mu(-)mu(-) is
performed with the D0 run II detector at the Fermilab
Tevatron. The analysis is based on a sample of inclusive
dimuon data collected at an energy of sqrt[s]=1.96 TeV,
corresponding to an integrated luminosity of 113 pb(-1). In
the absence of a signal, 95% confidence level mass limits of
M(H(+/-+/-)(L))>118.4 GeV/c(2) and M(H(+/-+/-)(R))>98.2
GeV/c(2) are set for left-handed and right-handed doubly
charged Higgs bosons, respectively, assuming 100% branching
into muon pairs.},
Doi = {10.1103/physrevlett.93.141801},
Key = {fds308161}
}
@article{fds374254,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei,
D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for doubly charged Higgs boson production in
multi-lepton final states using 139 fb - 1 of
proton–proton collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11578-9},
Abstract = {A search for pair production of doubly charged Higgs bosons
(H± ±), each decaying into a pair of prompt, isolated, and
highly energetic leptons with the same electric charge, is
presented. The search uses a proton–proton collision data
sample at a centre-of-mass energy of 13 TeV corresponding
to an integrated luminosity of 139 fb - 1 recorded by the
ATLAS detector during Run 2 of the Large Hadron Collider
(LHC). This analysis focuses on same-charge leptonic decays,
H±±→ℓ±ℓ′± where ℓ,ℓ′=e,μ,τ , in two-,
three-, and four-lepton channels, but only considers final
states which include electrons or muons. No evidence of a
signal is observed. Corresponding upper limits on the
production cross-section of a doubly charged Higgs boson are
derived, as a function of its mass m(H± ±) , at 95%
confidence level. Assuming that the branching ratios to each
of the possible leptonic final states are equal, B(H± ±→
e±e±) = B(H± ±→ e±μ±) = B(H± ±→ μ±μ±) =
B(H± ±→ e±τ±) = B(H± ±→ μ±τ±) = B(H± ±→
τ±τ±) = 1 / 6 , the observed (expected) lower limit on
the mass of a doubly charged Higgs boson is 1080 GeV
(1065 GeV) within the left-right symmetric type-II seesaw
model, which is the strongest limit to date produced by the
ATLAS Collaboration. Additionally, this paper provides the
first direct test of the Zee–Babu neutrino mass model at
the LHC, yielding an observed (expected) lower limit of
m(H± ±) = 900 GeV (880 GeV).},
Doi = {10.1140/epjc/s10052-023-11578-9},
Key = {fds374254}
}
@article{fds347473,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
Title = {Search for doubly charged Higgs boson production in
multi-lepton final states with the ATLAS detector using
proton-proton collisions at s = 13 TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {3},
Pages = {199},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5661-z},
Abstract = {A search for doubly charged Higgs bosons with pairs of
prompt, isolated, highly energetic leptons with the same
electric charge is presented. The search uses a
proton-proton collision data sample at a centre-of-mass
energy of 13 TeV corresponding to 36.1 fb - 1 of integrated
luminosity recorded in 2015 and 2016 by the ATLAS detector
at the LHC. This analysis focuses on the decays H ± ± →
e ± e ± , H ± ± → e ± μ ± and H ± ± → μ ± μ
± , fitting the dilepton mass spectra in several exclusive
signal regions. No significant evidence of a signal is
observed and corresponding limits on the production
cross-section and consequently a lower limit on m ( H ± ±
) are derived at 95% confidence level. With ℓ ± ℓ ± =
e ± e ± / μ ± μ ± / e ± μ ± , the observed lower
limit on the mass of a doubly charged Higgs boson only
coupling to left-handed leptons varies from 770 to 870 GeV
(850 GeV expected) for B ( H ± ± → ℓ ± ℓ ± ) =
100 % and both the expected and observed mass limits are
above 450 GeV for B ( H ± ± → ℓ ± ℓ ± ) = 10 %
and any combination of partial branching
ratios.},
Doi = {10.1140/epjc/s10052-018-5661-z},
Key = {fds347473}
}
@article{fds308159,
Author = {al, DAE},
Title = {Search for Doubly Charged Higgs Bosons Decaying to Dileptons
in pp-bar Collisions at sqrt[s]=1.96 TeV},
Journal = {Physical Review Letters},
Volume = {93},
Number = {22},
Pages = {221802},
Year = {2004},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.93.221802},
Abstract = {We present the results of a search for doubly charged Higgs
bosons (H±±) decaying to dileptons (ll') using ~ 240 pb-1
of pp-bar collision data collected by the CDF II experiment
at the Fermilab Tevatron. In our search region, given by
same-sign ll' mass mll'>80 GeV/c2 (100 GeV/c2 for ee
channel), we observe no evidence for H±± production. We
set limits on sigma (pp-bar-->H++H---- >l+l'+l-l'-) as a
function of the mass of the H±± and the chirality of its
couplings. Assuming exclusive same-sign dilepton decays, we
derive lower mass limits on H±±L of 133, 136, and 115
GeV/c2 in the ee, µµ, and eµ channels, respectively, and
a lower mass limit of 113 GeV/c2 on H±±R in the µµ
channel, all at the 95% confidence level.},
Doi = {10.1103/physrevlett.93.221802},
Key = {fds308159}
}
@article{fds307662,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for doubly charged Higgs bosons in like-sign dilepton
final states at √s = 7 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {12},
Publisher = {Springer Nature},
Year = {2012},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2244-2},
Abstract = {A search for doubly charged Higgs bosons decaying to pairs
of electrons and/or muons is presented. The search is
performed using a data sample corresponding to an integrated
luminosity of 4.7 fb−1of pp collisions at √s = 7 TeV
collected by the ATLAS detector at the LHC. Pairs of prompt,
isolated, high-pT leptons with the same electric charge
(e±e±, e±μ±, μ±μ±) are selected, and their
invariant mass distribution is searched for a narrow
resonance. No significant excess over Standard Model
background expectations is observed, and limits are placed
on the cross section times branching ratio for pair
production of doubly charged Higgs bosons. The masses of
doubly charged Higgs bosons are constrained depending on the
branching ratio into these leptonic final states. Assuming
pair production, coupling to left-handed fermions, and a
branching ratio of 100% for each final state, masses below
409 GeV, 375 GeV, and 398 GeV are excluded for e±e±,
e±μ±, and μ±μ±, respectively.},
Doi = {10.1140/epjc/s10052-012-2244-2},
Key = {fds307662}
}
@article{fds347446,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro,
V},
Title = {Search for doubly charged scalar bosons decaying into
same-sign W boson pairs with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {79},
Number = {1},
Pages = {58},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6500-y},
Abstract = {A search for doubly charged scalar bosons decaying into
<i>W</i> boson pairs is presented. It uses a data sample
from proton-proton collisions corresponding to an integrated
luminosity of 36.1 fb - 1 collected by the ATLAS detector
at the LHC at a centre-of-mass energy of 13 TeV in 2015 and
2016. This search is guided by a model that includes an
extension of the Higgs sector through a scalar triplet,
leading to a rich phenomenology that includes doubly charged
scalar bosons H ± ± . Those bosons are produced in pairs
in proton-proton collisions and decay predominantly into
electroweak gauge bosons H ± ± → W ± W ± .
Experimental signatures with several leptons, missing
transverse energy and jets are explored. No significant
deviations from the Standard Model predictions are found.
The parameter space of the benchmark model is excluded at
95% confidence level for H ± ± bosons with masses between
200 and 220 GeV.},
Doi = {10.1140/epjc/s10052-018-6500-y},
Key = {fds347446}
}
@article{fds30152,
Author = {A.V. Kotwal and D. Acosta et al.},
Title = {Search for Doubly-Charged Higgs Bosons Decaying to Dileptons
in proton-antiproton Collisions at sqrt(s) = 1.96
TeV},
Journal = {Physical Review Letters},
Volume = {93},
Number = {221802},
Year = {2004},
Month = {November},
Key = {fds30152}
}
@article{fds307692,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C},
Title = {Search for down-type fourth generation quarks with the ATLAS
detector in events with one lepton and hadronically decaying
W bosons.},
Journal = {Physical review letters},
Volume = {109},
Number = {3},
Pages = {032001},
Year = {2012},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.109.032001},
Abstract = {This Letter presents a search for pair production of heavy
down-type quarks decaying via b' → Wt in the lepton + jets
channel, as b'b' → W- tW+ t → bbW+ W- W+ W- → l±
νbbqqqqqq. In addition to requiring exactly one lepton,
large missing transverse momentum, and at least six jets,
the invariant mass of nearby jet pairs is used to identify
high transverse momentum W bosons. In data corresponding to
an integrated luminosity of 1.04 fb(-1) from pp
collisions at sqrt[s] = 7 TeV recorded with the ATLAS
detector, a heavy down-type quark with mass less than 480
GeV can be excluded at the 95% confidence
level.},
Doi = {10.1103/physrevlett.109.032001},
Key = {fds307692}
}
@article{fds356582,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V},
Title = {Search for electroweak diboson production in association
with a high-mass dijet system in semileptonic final states
in pp collisions at s =13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {100},
Number = {3},
Year = {2019},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.100.032007},
Abstract = {This paper reports on a search for electroweak diboson
(WW/WZ/ZZ) production in association with a high-mass dijet
system, using data from proton-proton collisions at a
center-of-mass energy of s=13 TeV. The data, corresponding
to an integrated luminosity of 35.5 fb-1, were recorded with
the ATLAS detector in 2015 and 2016 at the Large Hadron
Collider. The search is performed in final states in which
one boson decays leptonically, and the other boson decays
hadronically. The hadronically decaying W/Z boson is
reconstructed as either two small-radius jets or one
large-radius jet using jet substructure techniques. The
electroweak production of WW/WZ/ZZ in association with two
jets is measured with an observed (expected) significance of
2.7 (2.5) standard deviations, and the fiducial cross
section is measured to be 45.1±8.6(stat.)-14.6+15.9(syst.)
fb.},
Doi = {10.1103/PhysRevD.100.032007},
Key = {fds356582}
}
@article{fds356543,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob,
M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz,
L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira, RA},
Title = {Search for electroweak production of charginos and sleptons
decaying into final states with two leptons and missing
transverse momentum in √s=13 TeV pp collisions using the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {2},
Year = {2020},
Month = {February},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7594-6},
Abstract = {A search for the electroweak production of charginos and
sleptons decaying into final states with two electrons or
muons is presented. The analysis is based on 139 fb- 1 of
proton–proton collisions recorded by the ATLAS detector at
the Large Hadron Collider at s=13 TeV. Three
R-parity-conserving scenarios where the lightest neutralino
is the lightest supersymmetric particle are considered: the
production of chargino pairs with decays via either W bosons
or sleptons, and the direct production of slepton pairs. The
analysis is optimised for the first of these scenarios, but
the results are also interpreted in the others. No
significant deviations from the Standard Model expectations
are observed and limits at 95% confidence level are set on
the masses of relevant supersymmetric particles in each of
the scenarios. For a massless lightest neutralino, masses up
to 420 Ge are excluded for the production of the
lightest-chargino pairs assuming W-boson-mediated decays and
up to 1 TeV for slepton-mediated decays, whereas for
slepton-pair production masses up to 700 Ge are excluded
assuming three generations of mass-degenerate
sleptons.},
Doi = {10.1140/epjc/s10052-019-7594-6},
Key = {fds356543}
}
@article{fds332357,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Boos, EE and Borcherding, F and Brandt,
A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross,
A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV},
Title = {Search for electroweak production of single top Quarks in
pp̄ Collisions},
Journal = {Physical Review D},
Volume = {63},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2001},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.63.031101},
Abstract = {We present a search for electroweak production of single top
quarks in the electron+jets and muon+jets decay channels.
The measurements use ≃ 90 pb-1 of data from Run 1 of the
Fermilab Tevatron collider, collected at 1.8 TeV with the
DØ detector between 1992 and 1995. We use events that
include a tagging muon, implying the presence of a b jet, to
set an upper limit at the 95% confidence level on the cross
section for the s-channel process pp- → tb+X of 39 pb. The
upper limit for the t-channel process pp- → tqb+X is 58
pb.},
Doi = {10.1103/PhysRevD.63.031101},
Key = {fds332357}
}
@article{fds347484,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov,
G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini,
D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
TM and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu,
MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioară, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
Title = {Search for electroweak production of supersymmetric
particles in final states with two or three leptons at s =
13 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {12},
Pages = {995},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6423-7},
Abstract = {A search for the electroweak production of charginos,
neutralinos and sleptons decaying into final states
involving two or three electrons or muons is presented. The
analysis is based on 36.1 fb - 1 of s = 13 TeV
proton-proton collisions recorded by the ATLAS detector at
the Large Hadron Collider. Several scenarios based on
simplified models are considered. These include the
associated production of the next-to-lightest neutralino and
the lightest chargino, followed by their decays into final
states with leptons and the lightest neutralino via either
sleptons or Standard Model gauge bosons; direct production
of chargino pairs, which in turn decay into leptons and the
lightest neutralino via intermediate sleptons; and slepton
pair production, where each slepton decays directly into the
lightest neutralino and a lepton. No significant deviations
from the Standard Model expectation are observed and
stringent limits at 95% confidence level are placed on the
masses of relevant supersymmetric particles in each of these
scenarios. For a massless lightest neutralino, masses up to
580 GeV are excluded for the associated production of the
next-to-lightest neutralino and the lightest chargino,
assuming gauge-boson mediated decays, whereas for
slepton-pair production masses up to 500 GeV are excluded
assuming three generations of mass-degenerate
sleptons.},
Doi = {10.1140/epjc/s10052-018-6423-7},
Key = {fds347484}
}
@article{fds356695,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
O and Arnold, H and Arratia, M},
Title = {Search for electroweak production of supersymmetric states
in scenarios with compressed mass spectra at √s =13 TeV
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {97},
Number = {5},
Year = {2018},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.97.052010},
Abstract = {A search for electroweak production of supersymmetric
particles in scenarios with compressed mass spectra in final
states with two low-momentum leptons and missing transverse
momentum is presented. This search uses proton-proton
collision data recorded by the ATLAS detector at the Large
Hadron Collider in 2015-2016, corresponding to 36.1 fb-1 of
integrated luminosity at s=13 TeV. Events with same-flavor
pairs of electrons or muons with opposite electric charge
are selected. The data are found to be consistent with the
Standard Model prediction. Results are interpreted using
simplified models of R-parity-conserving supersymmetry in
which there is a small mass difference between the masses of
the produced supersymmetric particles and the lightest
neutralino. Exclusion limits at 95% confidence level are set
on next-to-lightest neutralino masses of up to 145 GeV for
Higgsino production and 175 GeV for wino production, and
slepton masses of up to 190 GeV for pair production of
sleptons. In the compressed mass regime, the exclusion
limits extend down to mass splittings of 2.5 GeV for
Higgsino production, 2 GeV for wino production, and 1 GeV
for slepton production. The results are also interpreted in
the context of a radiatively-driven natural supersymmetry
model with nonuniversal Higgs boson masses.},
Doi = {10.1103/PhysRevD.97.052010},
Key = {fds356695}
}
@article{fds308146,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Ronco, SD and D'Auria, S and Barbaro, PD and Cecco, SD and Lentdecker, GD and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and Pedis, DD and Derwent, PF and Dionisi, C and Dittmann,
JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch,
H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garcia-Sciveres, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, DW and Gerchtein, E and Giagu, S and Giannetti,
P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grosso-Pilcher, C and Grundler, U and Guenther, M and Costa, JGD and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, BY and Handler, R and Happacher, F and Hara, K and Hare, M and Harr,
RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays,
C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans,
D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Unel, MK and Karchin, PE and Kartal, S and Kato,
Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and LeCompte, T and Lee, J and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu,
T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons,
L and Lys, J and Lysak, R and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller,
JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, AS and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager, C and Pompoš, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine,
A and Rappoccio, S and Ratnikov, F and Ray, H and Reichold, A and Reisert,
B and Rekovic, V and Renton, P and Rescigno, M and Rimondi, F and Rinnert,
K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli,
S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz,
A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Denis, RS and Sakumoto, WK and Salamanna, G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan,
A},
Title = {Search for electroweak single-top-quark production in pp̄
collisions at √s = 1.96 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {1},
Pages = {012005-1-012005-7},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.012005},
Abstract = {We report on a search for standard model t-channel and
s-channel single-top quark production in pp̄ collisions at
a center of mass energy of 1.96 TeV. We use a data sample
corresponding to 162 pb-1 recorded by the upgraded collider
detector at Fermilab. We find no significant evidence for
electroweak top quark production and set upper limits at the
95% confidence level on the production cross section,
consistent with the standard model: 10.1 pb for the
t-channel, 13.6 pb for the s-channel and 17.8 pb for the
combined cross section of t- and s-channel. © 2005 The
American Physical Society.},
Doi = {10.1103/PhysRevD.71.012005},
Key = {fds308146}
}
@article{fds307772,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber,
T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
O and Benary, O and Benchekroun, D and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini,
I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement,
B},
Title = {Search for events with large missing transverse momentum,
jets, and at least two tau leptons in 7 TeV proton-proton
collision data with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {714},
Number = {2-5},
Pages = {180-196},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.06.055},
Abstract = {A search for events with large missing transverse momentum,
jets, and at least two tau leptons has been performed using
2 fb-1 of proton-proton collision data at s=7 TeV recorded
with the ATLAS detector at the Large Hadron Collider. No
excess above the Standard Model background expectation is
observed and a 95% CL upper limit on the visible cross
section for new phenomena is set, where the visible cross
section is defined by the product of cross section,
branching fraction, detector acceptance and event selection
efficiency. A 95% CL lower limit of 32 TeV is set on the
gauge-mediated supersymmetry breaking (GMSB) scale Λ
independent of tanβ. These limits provide the most
stringent tests to date in a large part of the considered
parameter space. © 2012.},
Doi = {10.1016/j.physletb.2012.06.055},
Key = {fds307772}
}
@article{fds308136,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, J-F and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerri, C and Cerrito, L and Chapman, J and Chen, C and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chu, ML and Chuang, S and Chung, JY and Chung, W-H and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway, J and Cooper, B and Cordelli, M and Cortiana, G and Cranshaw, J and Cuevas, J and Culbertson, R and Currat, C and Cyr, D and Dagenhart, D and Da Ronco and S and D'Auria, S and de Barbaro, P and De Cecco and S and De Lentdecker and G and Dell'Agnello, S and Dell'Orso, M and Demers, S and Demortier, L and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann,
JR and Doksus, P and Dominguez, A and Donati, S and Donega, M and Donini,
J and D'Onofrio, M and Dorigo, T and Drollinger, V and Ebina, K and Eddy,
N and Ely, R and Erbacher, R and Erdmann, M and Errede, D and Errede, S and Eusebi, R and Fang, H-C and Farrington, S and Fedorko, I and Feild, RG and Feindt, M and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flanagan, G and Flaugher, B and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch,
H and Fujii, Y and Furic, I and Gajjar, A and Gallas, A and Galyardt, J and Gallinaro, M and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes,
DW and Gerchtein, E and Giagu, S and Giannetti, P and Gibson, A and Gibson,
K and Ginsburg, C and Giolo, K and Giordani, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, D and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grosso-Pilcher, C and Grundler, U and Guenther, M and da Costa, JG and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harr, RF and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heider, E and Heinemann, B and Heinrich, J and Hennecke, M and Herndon,
M and Hill, C and Hirschbuehl, D and Hocker, A and Hoffman, KD and Holloway, A and Hou, S and Houlden, MA and Huffman, BT and Huang, Y and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Issever, C and Ivanov, A and Iwata, Y and Iyutin, B and James, E and Jang, D and Jarrell, J and Jeans, D and Jensen,
H and Jeon, EJ and Jones, M and Joo, KK and Jun, S and Junk, T and Kamon, T and Kang, J and Karagoz Unel and M and Karchin, PE and Kartal, S and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster,
B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, TH and Kim, YK and King, BT and Kirby, M and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kobayashi, H and Koehn, P and Kong, DJ and Kondo, K and Konigsberg, J and Kordas, K and Korn, A and Korytov, A and Kotelnikov, K and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreymer, A and Kroll, J and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kuznetsova, N and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lannon, K and Lath, A and Latino, G and Lauhakangas, R and Lazzizzera, I and Le, Y and Lecci, C and Lecompte, T and Lee, J and Lee, SW and Lefevre, R and Leonardo, N and Leone, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Liss, TM and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Malferrari, L and Manca, G and Marginean, R and Martin, M and Martin, A and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, M and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, PM and McNamara, P and NcNulty, R and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
A and Miao, T and Miladinovic, N and Miller, L and Miller, R and Miller,
JS and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Miyazaki, Y and Moggi, N and Mohr, B and Moore, R and Morello, M and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Munar, A and Murat, P and Nachtman, J and Nahn, S and Nakamura, I and Nakano, I and Napier, A and Napora, R and Naumov, D and Necula, V and Niell, F and Nielsen, J and Nelson, C and Nelson, T and Neu, C and Neubauer, MS and Newman-Holmes, C and Nicollerat, A-S and Nigmanov, T and Nodulman, L and Norniella, O and Oesterberg, K and Ogawa, T and Oh, SH and Oh, YD and Ohsugi, T and Okusawa, T and Oldeman, R and Orava, R and Orejudos, W and Pagliarone, C and Palencia, E and Palmonari, F and Paoletti, R and Papadimitriou, V and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Pauly, T and Paus, C and Pellett, D and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, KT and Plager,
C and Pompos, A and Pondrom, L and Pope, G and Poukhov, O and Prakoshyn, F and Pratt, T and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Rademacker, J and Rakitine, A and Rappoccio, S and Ratnikov, F and Ray,
H and Reichold, A and Reisert, B and Rekovic, V and Renton, P and Rescigno,
M and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Russ, J and Ruiz, A and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and St Denis and R and Sakumoto, WK and Salamanna,
G and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sarkar,
S and Sato, K and Savard, P and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semeria, F and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Siegrist, J and Siket, M and Sill, A and Sinervo, P and Sisakyan, A},
Title = {Search for excited and exotic electrons in the egamma decay
channel in pp collisions at sqrt[s] = 1.96
TeV.},
Journal = {Physical review letters},
Volume = {94},
Number = {10},
Pages = {101802},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.94.101802},
Abstract = {We present a search for excited and exotic electrons (e(*))
decaying to an electron and a photon, both with high
transverse momentum. We use 202 pb(-1) of data collected in
pp collisions at sqrt[s] = 1.96 TeV with the Collider
Detector at Fermilab II detector. No signal above standard
model expectation is seen for associated ee(*) production.
We discuss the e(*) sensitivity in the parameter space of
the excited electron mass M(e(*)) and the compositeness
energy scale Lambda. In the contact interaction model, we
exclude 132 GeV/c(2)<M(e(*))<879 GeV/c(2) for Lambda =
M(e(*)) at 95% confidence level (C.L.). In the
gauge-mediated model, we exclude 126 GeV/c(2) < M(e(*)) <
430 GeV/c(2) at 95% C.L. for the phenomenological coupling
f/Lambda approximately 10(-2) GeV-1.},
Doi = {10.1103/physrevlett.94.101802},
Key = {fds308136}
}
@article{fds362579,
Author = {Gerberich, H and Hays, C and Kotwal, A},
Title = {Search for Excited and Exotic Muons at CDF},
Year = {2006},
Month = {November},
Abstract = {We present a search for the production of excited or exotic
muons (mu*) via the reaction pbar + p -> mu* + mu -> mu
gamma + mu using 371/pb of data collected with the Run II
CDF detector. In this signature-based search, we look for a
resonance in the mu-gamma mass spectrum. The data are
compared to standard model and detector background
expectations, and with predictions of excited muon
production. We use these comparisons to set limits on the
mu* mass and compositeness scale Lambda in the contact
interaction and gauge-mediated models.},
Key = {fds362579}
}
@article{fds308116,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, JF and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Haim, EB and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carlsmith, D and Carosi, R and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri,
A and Cerrito, L and Chang, SH and Chapman, J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cruz, A and Almenar, CC and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'Onofrio, M and Dagenhart, D and Barbaro,
PD and Cecco, SD and Deisher, A and Lentdecker, GD and Dell'Orso, M and Paoli, FD and Demers, S and Demortier, L and Deng, J and Deninno, M and Pedis, DD and Derwent, PF and Giovanni, GPD and Ruzza, BD and Dionisi,
C and Dittmann, JR and DiTuro, P and Dörr, C and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo, LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Frisch, HJ and Furic, I and Gallinaro,
M and Galyardt, J and Garcia, JE and Sciveres, MG and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giokaris, N and Giolo, K and Giordani, M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev,
V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher, C and Group, RC and Grundler, U and Costa, JGD and Gunay-Unalan, Z and Haber, C and Hahn,
SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, BY and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Heijboer,
A and Heinemann, B and Heinrich, J and Herndon, M and Hidas, D and Hill,
CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden,
M and Hsu, SC and Huffman, BT and Hughes, RE and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon,
EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karchin, PE and Kato, Y and Kemp, Y and Kephart,
R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim,
HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kovalev, A and Kraan, A and Kraus, J and Kravchenko, I and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and LeCompte, T and Lee, J and Lee, YJ and Lee,
SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister,
A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti,
M and Loverre, P and Lu, RS and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maki, T and Maksimovic, P and Malde, S and Manca, G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin, V and Martínez, M and Maruyama, T and Mastrandrea, P and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta,
A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Mey, MVD and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Mitra, A and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Nachtman, J and Naganoma, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Nurse, E and Ogawa, T and Oh, SH and Oh,
YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn,
F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and Remortel, NV and Renton,
P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfiligoi, I and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet,
M},
Title = {Search for excited and exotic muons in the μy decay channel
in pp - collisions at s=1.96 TeV},
Journal = {Physical Review Letters},
Volume = {97},
Number = {19},
Pages = {191802},
Year = {2006},
ISSN = {0031-9007},
url = {http://www.ncbi.nlm.nih.gov/pubmed/17155615},
Abstract = {We search for excited and exotic muon states * using an
integrated luminosity of 371pb-1 of pp collision data at
s=1.96TeV. We search for associated production of * followed
by the decay *. We compare the data to model predictions as
a function of the mass of the excited muon M *, the
compositeness energy scale , and the gauge coupling factor
f. No signal above the standard model expectation is
observed. We exclude 107<M *<853GeV/c2 for =M * in the
contact interaction model, and 100<M *<410GeV/c2 for
f/=10-2GeV-1 in the gauge-mediated model, both at the 95%
confidence level. © 2006 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.97.191802},
Key = {fds308116}
}
@article{fds307581,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for excited electrons and muons in √s=8 TeV
proton-proton collisions with the ATLAS detector},
Journal = {New Journal of Physics},
Volume = {15},
Number = {9},
Pages = {093011-093011},
Publisher = {IOP Publishing},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1088/1367-2630/15/9/093011},
Abstract = {The ATLAS detector at the Large Hadron Collider is used to
search for excited electrons and excited muons in the
channel pp → ℓℓ* → ℓℓγ, assuming that excited
leptons are produced via contact interactions. The analysis
is based on 13 fb-1 of pp collisions at a centre-of-mass
energy of 8 TeV. No evidence for excited leptons is found,
and a limit is set at the 95% credibility level on the cross
section times branching ratio as a function of the
excited-lepton mass mℓ*. For mℓ* 0.8 TeV, the respective
upper limits on σB(ℓ* → ℓγ) are 0.75 and 0.90 fb for
the e* and μ* searches. Limits on σB are converted into
lower bounds on the compositeness scale Λ. In the special
case where Λ = m ℓ*, excited-electron and excited-muon
masses below 2.2 TeV are excluded. © CERN
2013.},
Doi = {10.1088/1367-2630/15/9/093011},
Key = {fds307581}
}
@article{fds356580,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira, RA and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arling,
JH},
Title = {Search for excited electrons singly produced in
proton–proton collisions at √s=13Te with the ATLAS
experiment at the LHC},
Journal = {European Physical Journal C},
Volume = {79},
Number = {9},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7295-1},
Abstract = {A search for excited electrons produced in pp collisions at
s = 13 Te via a contact interaction qq¯ → ee∗ is
presented. The search uses 36.1 fb- 1 of data collected in
2015 and 2016 by the ATLAS experiment at the Large Hadron
Collider. Decays of the excited electron into an electron
and a pair of quarks (eqq¯) are targeted in final states
with two electrons and two hadronic jets, and decays via a
gauge interaction into a neutrino and a W boson (νW) are
probed in final states with an electron, missing transverse
momentum, and a large-radius jet consistent with a
hadronically decaying W boson. No significant excess is
observed over the expected backgrounds. Upper limits are
calculated for the pp→ ee∗→ eeqq¯ and pp→ ee∗→
eνW production cross sections as a function of the excited
electron mass me∗ at 95% confidence level. The limits are
translated into lower bounds on the compositeness scale
parameter Λ of the model as a function of me∗. For
me∗<0.5 Te, the lower bound for Λ is 11 Te. In the
special case of me∗=Λ, the values of me∗<4.8 Te are
excluded. The presented limits on Λ are more stringent than
those obtained in previous searches.},
Doi = {10.1140/epjc/s10052-019-7295-1},
Key = {fds356580}
}
@article{fds307735,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for excited leptons in proton-proton collisions at
√s=7TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.85.072003},
Abstract = {The ATLAS detector is used to search for excited leptons in
the electromagnetic radiative decay channel *→γ. Results
are presented based on the analysis of pp collisions at a
center-of-mass energy of 7 TeV corresponding to an
integrated luminosity of 2.05fb-1. No evidence for excited
leptons is found, and limits are set on the compositeness
scale Λ as a function of the excited lepton mass m *. In
the special case where Λ=m *, excited electron and muon
masses below 1.87 TeV and 1.75 TeV are excluded at 95% C.L.,
respectively. © 2012 CERN.},
Doi = {10.1103/PhysRevD.85.072003},
Key = {fds307735}
}
@article{fds308047,
Author = {Aaltonen, T and Abulencia, A and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Amerio, S and Amidei, D and Anastassov, A and Anikeev,
K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Behari,
S and Bellettini, G and Bellinger, J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Carrillo, S and Carlsmith, D and Caron, B and Carosi, R and Carron,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Cilijak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Daronco, S and Datta, M and D'Auria, S and Davies, T and Dagenhart, D and de Barbaro, P and De
Cecco, S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'orso, M and Delli Paoli and F and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Dörr,
C and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
M and Galyardt, J and Garcia, JE and Garberson, F and Garfinkel, AF and Gay, C and Gerberich, H and Gerdes, D and Giagu, S and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, C and Giokaris, N and Giordani,
M and Giromini, P and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson,
C and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl,
D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel,
U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraan, AC and Kraus,
J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Lin,
C and Lin, CS and Lindgren, M and Lipeles, E and Lister, A and Litvintsev,
DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys,
J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli, F and Marginean,
R and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty,
R and Mehta, A and Mehtala, P and Menzemer, S and Menzione, A and Merkel,
P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles,
J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher,
G and Miyamoto, A and Moed, S and Moggi, N and Mohr, B and Moon, CS and Moore,
R and Morello, M and Fernandez, PM and Mülmenstädt, J and Mukherjee,
A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone,
C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta,
G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin,
R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov,
A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar,
S and Sartori, L and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano,
A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyrla, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard, PF and Sherman, D and Shimojima, M and Shochet,
M},
Title = {Search for exclusive gammagamma production in Hadron-Hadron
collisions.},
Journal = {Physical review letters},
Volume = {99},
Number = {24},
Pages = {242002},
Year = {2007},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.99.242002},
Abstract = {We have searched for exclusive gammagamma production in
proton-antiproton collisions at sqrt[s]=1.96 TeV, using 532
pb(-1) of integrated luminosity taken by the run II Collider
Detector at Fermilab. The event signature requires two
electromagnetic showers, each with transverse energy E(T)>5
GeV and pseudorapidity |eta|<1.0, with no other particles
detected in the event. Three candidate events are observed.
We discuss the consistency of the three events with
gammagamma, pi(0)pi(0), or eta eta production. The
probability that other processes fluctuate to >or=3 events
is 1.7x10(-4). An upper limit on the cross section of pp-->p
+ gammagamma + p production is set at 410 fb with 95%
confidence level.},
Doi = {10.1103/physrevlett.99.242002},
Key = {fds308047}
}
@article{fds356675,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for exclusive Higgs and Z boson decays to ϕγ and
ργ with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {7},
Year = {2018},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2018)127},
Abstract = {A search for the exclusive decays of the Higgs and Z bosons
to a ϕ or ρ meson and a photon is performed with a pp
collision data sample corresponding to an integrated
luminosity of up to 35.6 fb−1 collected at s=13 TeV with
the ATLAS detector at the CERN Large Hadron Collider. These
decays have been suggested as a probe of the Higgs boson
couplings to light quarks. No significant excess of events
is observed above the background, as expected from the
Standard Model. Upper limits at 95% confidence level were
obtained on the branching fractions of the Higgs boson
decays to ϕγ and ργ of 4.8 × 10−4 and 8.8 × 10−4,
respectively. The corresponding 95% confidence level upper
limits for the Z boson decays are 0.9 × 10−6 and 25 ×
10−6 for ϕγ and ργ, respectively.[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP07(2018)127},
Key = {fds356675}
}
@article{fds375876,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for exclusive Higgs and Z boson decays to ωγ and
Higgs boson decays to K⁎γ with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {847},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138292},
Abstract = {Searches for the exclusive decays of the Higgs boson to an
ω meson and a photon or a K⁎ meson and a photon can probe
flavour-conserving and flavour-violating Higgs boson
couplings to light quarks, respectively. Searches for these
decays, along with the analogous Z boson decay to an ω
meson and a photon, are performed with a pp collision data
sample corresponding to integrated luminosities of up to 134
fb−1 collected at s=13 TeV with the ATLAS detector at the
CERN Large Hadron Collider. The obtained 95%
confidence-level upper limits on the respective branching
fractions are B(H→ωγ)<5.5×10−4, B(H→K⁎γ)<2.2×10−4
and B(Z→ωγ)<3.9×10−6. The limits for H→ωγ and
Z→ωγ are 370 times and 140 times the Standard Model
expected values, respectively. The result for Z→ωγ
corresponds to a two-orders-of-magnitude improvement over
the limit obtained by the DELPHI experiment at
LEP.},
Doi = {10.1016/j.physletb.2023.138292},
Key = {fds375876}
}
@article{fds307975,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi,
F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley,
M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld,
B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori,
L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell,
M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and Di Canto and A and di Giovanni, GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest, R and Frank, MJ and Franklin, M and Freeman,
JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Garosi, P and Genser, K and Gerberich,
H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele,
A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
da Costa, J and Gunay-Unalan, Z and Haber, C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas,
D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung,
JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko,
S and Knuteson, B and Ko, BR and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee, HS and Lee,
SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Pagan Griso and S and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pinera, L and Pinfold, J and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Pueschel, E and Punzi, G and Pursley, J and Rademacker,
J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton, P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto, WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel,
S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla, A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sinervo,
P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M},
Title = {Search for exclusive Z-boson production and observation of
high-mass pp[over ]-->pgammagammap[over ]-->pl;{+}l;{-}p[over
] events in pp[over ] collisions at sqrt[s]=1.96
TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {22},
Pages = {222002},
Year = {2009},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.102.222002},
Abstract = {This Letter presents a search for exclusive Z boson
production in proton-antiproton collisions at sqrt[s]=1.96
TeV, using the CDF II detector. No exclusive Z-->l;{+}l;{-}
candidates are observed and the first upper limit on the
exclusive Z cross section in hadron collisions is found to
be sigma_{excl}(Z)<0.96 pb at 95% confidence level. In
addition, eight candidate exclusive dilepton events from the
process pp[over ]-->pgammagammap[over ]-->pl;{+}l;{-}p[over
] are observed, and a measurement of the cross section for
M_{ll}>40 GeV/c;{2} and |eta_{l}|<4 is found to be
sigma=0.24_{-0.10};{+0.13} pb, which is consistent with the
standard model prediction.},
Doi = {10.1103/physrevlett.102.222002},
Key = {fds307975}
}
@article{fds308071,
Author = {Abulencia, and A, and others},
Title = {Search for Exotic $S=-2$ Baryons in $p\bar{p}$ Collisions at
$\sqrt{s}=1.96\,TeV$},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {3},
Pages = {032003},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.032003},
Abstract = {A search for a manifestly exotic S=-2 baryon state decaying
to Xi-pi-, and its neutral partner decaying to Xi-pi+, has
been performed using 220 pb-1 of p[overline p] collisions at
sqrt(s)=1.96 TeV collected by the Collider Detector at
Fermilab. The Xi- trajectories were measured in a silicon
tracker before their decay, resulting in a sample with low
background and excellent position resolution. No evidence
was found for S=-2 pentaquark candidates in the invariant
mass range of 1600--2100 MeV/c2. Upper limits on the product
of pentaquark production cross section times its branching
fraction to Xi-pi+,-, relative to the cross section of the
well-established Xi(1530) resonance, are presented for
neutral and doubly negative candidates with pT>2 GeV/c and
|y|},
Doi = {10.1103/PhysRevD.75.032003},
Key = {fds308071}
}
@article{fds361805,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala,
J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF},
Title = {Search for exotic decays of the Higgs boson into b b¯ and
missing transverse momentum in pp collisions at √s = 13
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2022},
Number = {1},
Year = {2022},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2022)063},
Abstract = {A search for the exotic decay of the Higgs boson (H) into a
bb¯ resonance plus missing transverse momentum is
described. The search is performed with the ATLAS detector
at the Large Hadron Collider using 139 fb−1 of pp
collisions at s = 13 TeV. The search targets events from ZH
production in an NMSSM scenario where H → χ~20χ~10, with
χ~20→aχ~10, where a is a light pseudoscalar Higgs boson
and χ~1,20 are the two lightest neutralinos. The decay of
the a boson into a pair of b-quarks results in a peak in the
dijet invariant mass distribution. The final-state signature
consists of two leptons, two or more jets, at least one of
which is identified as originating from a b-quark, and
missing transverse momentum. Observations are consistent
with Standard Model expectations and upper limits are set on
the product of cross section times branching ratio for a
three-dimensional scan of the masses of the χ~20, χ~10 and
a boson. [Figure not available: see fulltext.]},
Doi = {10.1007/JHEP01(2022)063},
Key = {fds361805}
}
@article{fds360769,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
Title = {Search for exotic decays of the Higgs boson into long-lived
particles in pp collisions at √s = 13 TeV using displaced
vertices in the ATLAS inner detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2021)229},
Abstract = {A novel search for exotic decays of the Higgs boson into
pairs of long-lived neutral particles, each decaying into a
bottom quark pair, is performed using 139 fb−1 of s = 13
TeV proton-proton collision data collected with the ATLAS
detector at the LHC. Events consistent with the production
of a Higgs boson in association with a leptonically decaying
Z boson are analysed. Long-lived particle (LLP) decays are
reconstructed from inner-detector tracks as displaced
vertices with high mass and track multiplicity relative to
Standard Model processes. The analysis selection requires
the presence of at least two displaced vertices, effectively
suppressing Standard Model backgrounds. The residual
background contribution is estimated using a data-driven
technique. No excess over Standard Model predictions is
observed, and upper limits are set on the branching ratio of
the Higgs boson to LLPs. Branching ratios above 10% are
excluded at 95% confidence level for LLP mean proper
lifetimes cτ as small as 4 mm and as large as 100 mm. For
LLP masses below 40 GeV, these results represent the most
stringent constraint in this lifetime regime. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP11(2021)229},
Key = {fds360769}
}
@article{fds307606,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Search for extra dimensions in diphoton events from
proton-proton collisions at √s= 7 TeV in the ATLAS
detector at the LHC},
Journal = {New Journal of Physics},
Volume = {15},
Number = {4},
Pages = {043007-043007},
Publisher = {IOP Publishing},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1088/1367-2630/15/4/043007},
Abstract = {The large difference between the Planck scale and the
electroweak scale, known as the hierarchy problem, is
addressed in certain models through the postulate of extra
spatial dimensions. A search for evidence of extra spatial
dimensions in the diphoton channel has been performed using
the full set of proton-proton collisions at √s = 7 TeV
recorded in 2011 with the ATLAS detector at the CERN Large
Hadron Collider. This dataset corresponds to an integrated
luminosity of 4.9 fb1. The diphoton invariant mass spectrum
is observed to be in good agreement with the Standard Model
expectation. In the context of the model proposed by
Arkani-Hamed, Dimopoulos and Dvali, 95% confidence level
lower limits of between 2.52 and 3.92 TeV are set on the
ultraviolet cutoff scale MS depending on the number of extra
dimensions and the theoretical formalism used. In the
context of the Randall-Sundrum model, a lower limit of 2.06
(1.00) TeV at 95% confidence level is set on the mass of the
lightest graviton for couplings of k/MPl = 0.1(0.01).
Combining with the ATLAS dilepton searches based on the 2011
data, the 95% confidence level lower limit on the
Randall-Sundrum graviton mass is further tightened to 2.23
(1.03) TeV for k/ MPl= 0.1(0.01).© CERN 2013 for the
benefit of the ATLAS Collaboration.},
Doi = {10.1088/1367-2630/15/4/043007},
Key = {fds307606}
}
@article{fds307732,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov,
A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B},
Title = {Search for extra dimensions using diphoton events in 7 TeV
proton-proton collisions with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {710},
Number = {4-5},
Pages = {538-556},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.03.022},
Abstract = {Using data recorded in 2011 with the ATLAS detector at the
Large Hadron Collider, a search for evidence of extra
spatial dimensions has been performed through an analysis of
the diphoton final state. The analysis uses data
corresponding to an integrated luminosity of 2.12fb-1 of
s=7TeV proton-proton collisions. The diphoton invariant mass
(mγγ) spectrum is observed to be in good agreement with
the expected Standard Model background. In the large extra
dimension scenario of Arkani-Hamed, Dimopoulos and Dvali,
the results provide 95% CL lower limits on the fundamental
Planck scale between 2.27 and 3.53 TeV, depending on the
number of extra dimensions and the theoretical formalism
used. The results also set 95% CL lower limits on the
lightest Randall-Sundrum graviton mass of between 0.79 and
1.85 TeV, for values of the dimensionless coupling k/-1 Pl
varying from 0.01 to 0.1. Combining with previously
published ATLAS results from the dielectron and dimuon final
states, the 95% CL lower limit on the Randall-Sundrum
graviton mass for k/M-1Pl=0.01 (0.1) is 0.80 (1.95) TeV. ©
2012 CERN.},
Doi = {10.1016/j.physletb.2012.03.022},
Key = {fds307732}
}
@article{fds307727,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for FCNC single top-quark production at √s=7 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {712},
Number = {4-5},
Pages = {351-369},
Publisher = {Elsevier BV},
Year = {2012},
Month = {June},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.05.022},
Abstract = {A search for the production of single top-quarks via
flavour-changing neutral-currents is presented. Data
collected with the ATLAS detector at a centre-of-mass energy
of s=7 TeV, corresponding to an integrated luminosity of
2.05 fb−1, are used. Candidate events with a semileptonic
top-quark decay signature are classified as signal- or
background-like events by using several kinematic variables
as input to a neural network. No signal is observed in the
neural network output distribution and a Bayesian upper
limit is placed on the production cross-section. The
observed upper limit at 95% confidence level on the
cross-section multiplied by the t→Wb branching fraction is
measured to be σqg→t×B(t→Wb)<3.9 pb. This upper limit
is converted using a model-independent approach into upper
limits on the coupling strengths κugt/Λ<6.9⋅10−3
TeV−1 and κcgt/Λ<1.6⋅10−2 TeV−1, where Λ is the
new physics scale, and on the branching fractions
B(t→ug)<5.7⋅10−5 and B(t→cg)<2.7⋅10−4.},
Doi = {10.1016/j.physletb.2012.05.022},
Key = {fds307727}
}
@booklet{Abbott98l,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Search for first generation scalar leptoquark pairs in pp
collisions at √ s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {80},
Number = {10},
Pages = {2051-2056},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.2051},
Abstract = {We have searched for first generation scalar leptoquark (LQ)
pairs in the ev + jets channel using pp collider data (∫L
dt ≈ 115pb-1) collected by the D0 experiment at the
Fermilab Tevatron during 1992-1996. The analysis yields no
candidate events. We combine the results with those from the
ee + jets vv + jets channels to obtain 95% confidence level
(C.L.) upper limits on the LQ pair production cross section
as a function of mass and of β, the branching fraction to a
charged lepton. Comparing with the next-to-leading order
theory, we set 95% C.L. lower limits on the LQ mass of 225,
204, and 79 GeV/c2 for β = 1, 1/2, and 0, respectively. ©
1998 The American Physical Society.},
Doi = {10.1103/PhysRevLett.80.2051},
Key = {Abbott98l}
}
@article{fds307734,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov,
A},
Title = {Search for first generation scalar leptoquarks in pp
collisions at s=7 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {709},
Number = {3},
Pages = {158-176},
Publisher = {Elsevier BV},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2012.02.004},
Abstract = {We report a search for first generation scalar leptoquarks
using 1.03fb-1 of proton-proton collisions data produced by
the Large Hadron Collider at s=7 TeV and recorded by the
ATLAS experiment. Leptoquarks are sought via their decay
into an electron or neutrino and a quark, producing events
with two oppositely charged electrons and at least two jets,
or events with an electron, missing transverse momentum and
at least two jets. Control data samples are used to validate
background predictions from Monte Carlo simulation. In the
signal region, the observed event yields are consistent with
the background expectations. We exclude at 95% confidence
level the production of first generation scalar leptoquark
with masses mLQ<660(607) GeV when assuming the branching
fraction of a leptoquark to a charged lepton is equal to 1.0
(0.5). © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.02.004},
Key = {fds307734}
}
@article{fds308186,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot,
L},
Title = {Search for first-generation scalar and vector
leptoquarks},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {64},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2001},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.64.092004},
Abstract = {We describe a search for the pair production of
first-generation scalar and vector leptoquarks in the
[Formula Presented] and [Formula Presented] channels by the
DØ Collaboration. The data are from the 1992–1996
[Formula Presented] run at [Formula Presented] at the
Fermilab Tevatron collider. We find no evidence for
leptoquark production; in addition, no kinematically
interesting events are observed using relaxed selection
criteria. The results from the [Formula Presented] and
[Formula Presented] channels are combined with those from a
previous DØ analysis of the [Formula Presented] channel to
obtain 95% confidence level (C.L.) upper limits on the
leptoquark pair-production cross section as a function of
mass and of [Formula Presented] the branching fraction to a
charged lepton. These limits are compared to
next-to-leading-order theory to set 95% C.L. lower limits on
the mass of a first-generation scalar leptoquark of 225,
204, and 79 [Formula Presented] for [Formula Presented]
[Formula Presented] and 0, respectively. For vector
leptoquarks with gauge (Yang-Mills) couplings, 95% C.L.
lower limits of 345, 337, and 206 [Formula Presented] are
set on the mass for [Formula Presented] [Formula Presented]
and 0, respectively. Mass limits for vector leptoquarks are
also set for anomalous vector couplings. © 2001 The
American Physical Society.},
Doi = {10.1103/PhysRevD.64.092004},
Key = {fds308186}
}
@article{fds308115,
Author = {Acosta, and D, and others},
Title = {Search for first-generation scalar leptoquarks in pp-bar
collisions at sqrt[s]=1.96 TeV},
Journal = {Phys. Rev.},
Volume = {D72},
Number = {5},
Pages = {051107},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.73.051102},
Abstract = {Results on a search for pair production of second-generation
scalar leptoquark in pp̄ collisions at s=1.96TeV are
reported. The data analyzed were collected by the CDF
detector during the 2002-2003 Tevatron Run II and correspond
to an integrated luminosity of 198pb-1. Leptoquarks (LQ) are
sought through their decay into (charged) leptons and
quarks, with final state signatures represented by two muons
and jets and one muon, large transverse missing energy and
jets. We observe no evidence for LQ production and derive
95% C.L. upper limits on the LQ production cross sections as
well as lower limits on their mass as a function of β,
where β is the branching fraction for LQ→μq. © 2006 The
American Physical Society.},
Doi = {10.1103/PhysRevD.73.051102},
Key = {fds308115}
}
@article{fds356668,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A},
Title = {Search for flavor-changing neutral currents in top quark
decays t →Hc and t →Hu in multilepton final states in
proton-proton collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {98},
Number = {3},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.98.032002},
Abstract = {Flavor-changing neutral currents are not present in the
Standard Model at tree level and are suppressed in loop
processes by the unitarity of the Cabibbo-Kobayashi-Maskawa
matrix; the corresponding rates for top quark decay
processes are experimentally unobservable. Extensions of the
Standard Model can generate new flavor-changing neutral
current processes, leading to signals which, if observed,
would be unambiguous evidence of new interactions. A data
set corresponding to an integrated luminosity of 36.1 fb-1
of pp collisions at a center-of-mass energy of s=13 TeV
recorded with the ATLAS detector at the Large Hadron
Collider is used to search for top quarks decaying to up or
charm quarks with the emission of a Higgs boson, with
subsequent Higgs boson decay to final states with at least
one electron or muon. No signal is observed and limits on
the branching fractions B(t→Hc)<0.16% and B(t→Hu)<0.19%
at 95% confidence level are obtained (with expected limits
of 0.15% in both cases).},
Doi = {10.1103/PhysRevD.98.032002},
Key = {fds356668}
}
@article{fds373910,
Author = {Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Sharma, AS and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Duran Yildiz and H and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco,
L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo Martinez and N and Portales, L and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem,
L and Wingerter-Seez, I and Abulaiti, Y and Bhopatkar, VS and Chekanov,
S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love,
J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van
Gemmeren, P and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Delitzsch, CM and Ghosh, A and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand, HK and Little, JD and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas,
L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Gazis, EN and Gkountoumis, P and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Panchal, DK and Roy, A and Unal, M and Webb, AF and Adiguzel,
A},
Title = {Search for flavor-changing neutral-current couplings between
the top quark and the Z boson with proton-proton
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032019},
Abstract = {A search for flavor-changing neutral-current couplings
between a top quark, an up or charm quark, and a Formula
Presented boson is presented, using proton-proton collision
data at Formula Presented collected by the ATLAS detector at
the Large Hadron Collider. The analyzed data set corresponds
to an integrated luminosity of Formula Presented. The search
targets both single-top-quark events produced as Formula
Presented (with Formula Presented, Formula Presented) and
top-quark-pair events, with one top quark decaying through
the Formula Presented channel. The analysis considers events
with three leptons (electrons or muons), a Formula
Presented-tagged jet, possible additional jets, and missing
transverse momentum. The data are found to be consistent
with the background-only hypothesis and 95% confidence-level
limits on the Formula Presented branching ratios, assuming
only tensor operators of the Standard Model effective field
theory framework contribute to the Formula Presented
vertices. These are Formula Presented (Formula Presented)
for Formula Presented (Formula Presented) for a left-handed
Formula Presented coupling, and Formula Presented (Formula
Presented) in the case of a right-handed coupling. These
results are interpreted as 95% CL upper limits on the
strength of the corresponding couplings, yielding limits for
Formula Presented and Formula Presented (Formula Presented
and Formula Presented) of 0.15 (0.16), and limits for
Formula Presented and Formula Presented (Formula Presented
and Formula Presented) of 0.22 (0.21), assuming a
new-physics energy scale Formula Presented of 1
TeV.},
Doi = {10.1103/PhysRevD.108.032019},
Key = {fds373910}
}
@article{fds313611,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for flavour-changing neutral current top quark decays
t → Hq in pp collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {12},
Pages = {1-65},
Publisher = {Springer Nature},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2015)061},
Abstract = {Abstract: A search for flavour-changing neutral current
decays of a top quark to an uptype quark (q = u, c) and the
Standard Model Higgs boson, where the Higgs boson decays
to(Formula Presented.), is presented. The analysis searches
for top quark pair events in which one top quark decays to
Wb, with the W boson decaying leptonically, and the other
top quark decays to Hq. The search is based on pp collisions
at (Formula Presented.) TeV recorded in 2012 with the ATLAS
detector at the CERN Large Hadron Collider and uses an
integrated luminosity of 20.3 fb−1. Data are analysed in
the lepton-plus-jets final state, characterised by an
isolated electron or muon and at least four jets. The search
exploits the high multiplicity of b-quark jets
characteristic of signal events, and employs a likelihood
discriminant that uses the kinematic differences between the
signal and the background, which is dominated by (Formula
Presented.) decays. No significant excess of events above
the background expectation is found, and observed (expected)
95% CL upper limits of 0.56% (0.42%) and 0.61% (0.64%) are
derived for the t → Hc and t → Hu branching ratios
respectively. The combination of this search with other
ATLAS searches in the H → γγ and H → WW*, ττ decay
modes significantly improves the sensitivity, yielding
observed (expected) 95% CL upper limits on the t → Hc and
t → Hu branching ratios of 0.46% (0.25%) and 0.45% (0.29%)
respectively. The corresponding combined observed (expected)
upper limits on the |λtcH| and |λtuH| couplings are 0.13
(0.10) and 0.13 (0.10) respectively. These are the most
restrictive direct bounds on tqH interactions measured so
far.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP12(2015)061},
Key = {fds313611}
}
@article{fds356676,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for flavour-changing neutral current top-quark decays
t → qZ in proton-proton collisions at √s=13 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {7},
Year = {2018},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2018)176},
Abstract = {A search for flavour-changing neutral-current processes in
top-quark decays is presented. Data collected with the ATLAS
detector from proton-proton collisions at the Large Hadron
Collider at a centre-of-mass energy of s=13 TeV,
corresponding to an integrated luminosity of 36.1 fb−1,
are analysed. The search is performed using top-quark pair
events, with one top quark decaying through the t → qZ (q
= u, c) flavour-changing neutral-current channel, and the
other through the dominant Standard Model mode t → bW.
Only Z boson decays into charged leptons and leptonic W
boson decays are considered as signal. Consequently, the
final-state topology is characterized by the presence of
three isolated charged leptons (electrons or muons), at
least two jets, one of the jets originating from a b-quark,
and missing transverse momentum from the undetected
neutrino. The data are consistent with Standard Model
background contributions, and at 95% confidence level the
search sets observed (expected) upper limits of 1.7 ×
10−4 (2.4 × 10−4) on the t → uZ branching ratio and
2.4 × 10−4 (3.2 × 10−4) on the t → cZ branching
ratio, constituting the most stringent limits to
date.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP07(2018)176},
Key = {fds356676}
}
@article{fds347516,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T},
Title = {Search for flavour-changing neutral current top-quark decays
to [Formula: see text] in [Formula: see text] collision data
collected with the ATLAS detector at [Formula: see
text] TeV.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {12},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3851-5},
Abstract = {A search for the flavour-changing neutral-current decay
[Formula: see text] is presented. Data collected by the
ATLAS detector during 2012 from proton-proton collisions at
the Large Hadron Collider at a centre-of-mass energy of
[Formula: see text] TeV, corresponding to an integrated
luminosity of 20.3 fb[Formula: see text], are analysed.
Top-quark pair-production events with one top quark decaying
through the [Formula: see text] ([Formula: see text])
channel and the other through the dominant Standard Model
mode [Formula: see text] are considered as signal. Only the
decays of the <i>Z</i> boson to charged leptons and leptonic
<i>W</i> boson decays are used. No evidence for a signal is
found and an observed (expected) upper limit on the
[Formula: see text] branching ratio of [Formula: see text]
([Formula: see text]) is set at the 95 % confidence
level.},
Doi = {10.1140/epjc/s10052-015-3851-5},
Key = {fds347516}
}
@article{fds356545,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Search for flavour-changing neutral currents in processes
with one top quark and a photon using 81 fb−1
of pp collisions at s=13TeV with the ATLAS
experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {800},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2019.135082},
Abstract = {A search for flavour-changing neutral current (FCNC) events
via the coupling of a top quark, a photon, and an up or
charm quark is presented using 81 fb−1 of proton–proton
collision data taken at a centre-of-mass energy of 13 TeV
with the ATLAS detector at the LHC. Events with a photon, an
electron or muon, a b-tagged jet, and missing transverse
momentum are selected. A neural network based on kinematic
variables differentiates between events from signal and
background processes. The data are consistent with the
background-only hypothesis, and limits are set on the
strength of the tqγ coupling in an effective field theory.
These are also interpreted as 95% CL upper limits on the
cross section for FCNC tγ production via a left-handed
(right-handed) tuγ coupling of 36 fb (78 fb) and on the
branching ratio for t→γu of 2.8×10−5 (6.1×10−5). In
addition, they are interpreted as 95% CL upper limits on the
cross section for FCNC tγ production via a left-handed
(right-handed) tcγ coupling of 40 fb (33 fb) and on the
branching ratio for t→γc of 22×10−5
(18×10−5).},
Doi = {10.1016/j.physletb.2019.135082},
Key = {fds356545}
}
@article{fds372127,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Search for flavour-changing neutral-current couplings
between the top quark and the photon with the ATLAS detector
at s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {842},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1016/j.physletb.2022.137379},
Abstract = {This letter documents a search for flavour-changing neutral
currents (FCNCs), which are strongly suppressed in the
Standard Model, in events with a photon and a top quark with
the ATLAS detector. The analysis uses data collected in pp
collisions at s=13 TeV during Run 2 of the LHC,
corresponding to an integrated luminosity of 139 fb−1.
Both FCNC top-quark production and decay are considered. The
final state consists of a charged lepton, missing transverse
momentum, a b-tagged jet, one high-momentum photon and
possibly additional jets. A multiclass deep neural network
is used to classify events either as signal in one of the
two categories, FCNC production or decay, or as background.
No significant excess of events over the background
prediction is observed and 95% CL upper limits are placed on
the strength of left- and right-handed FCNC interactions.
The 95% CL bounds on the branching fractions for the FCNC
top-quark decays, estimated (expected) from both top-quark
production and decay, are B(t→uγ)<0.85(0.88−0.25+0.37)×10−5
and B(t→cγ)<4.2(3.40−0.95+1.35)×10−5 for a
left-handed tqγ coupling, and B(t→uγ)<1.2(1.20−0.33+0.50)×10−5
and B(t→cγ)<4.5(3.70−1.03+1.47)×10−5 for a
right-handed coupling.},
Doi = {10.1016/j.physletb.2022.137379},
Key = {fds372127}
}
@article{fds363185,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C},
Title = {Search for flavour-changing neutral-current interactions of
a top quark and a gluon in pp collisions at √s=13 TeV with
the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {4},
Year = {2022},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10182-7},
Abstract = {A search is presented for the production of a single top
quark via left-handed flavour-changing neutral-current
(FCNC) interactions of a top quark, a gluon and an up or
charm quark. Two production processes are considered: u+
g→ t and c+ g→ t. The analysis is based on
proton–proton collision data taken at a centre-of-mass
energy of 13 TeV with the ATLAS detector at the LHC. The
data set corresponds to an integrated luminosity of 139 fb-
1. Events with exactly one electron or muon, exactly one
b-tagged jet and missing transverse momentum are selected,
resembling the decay products of a singly produced top
quark. Neural networks based on kinematic variables
differentiate between events from the two signal processes
and events from background processes. The measured data are
consistent with the background-only hypothesis, and limits
are set on the production cross-sections of the signal
processes: σ(u+g→t)×B(t→Wb)×B(W→ℓν)<3.0pb and
σ(c+g→t)×B(t→Wb)×B(W→ℓν)<4.7pb at the 95%
confidence level, with B(W→ ℓν) = 0.325 being the sum
of branching ratios of all three leptonic decay modes of the
W boson. Based on the framework of an effective field
theory, the cross-section limits are translated into limits
on the strengths of the tug and tcg couplings occurring in
the theory: |CuGut|/Λ2<0.057TeV- 2 and |CuGct|/Λ2<0.14TeV-
2. These bounds correspond to limits on the branching ratios
of FCNC-induced top-quark decays: B(t→ u+ g) < 0.61 × 10
- 4 and B(t→ c+ g) < 3.7 × 10 - 4.},
Doi = {10.1140/epjc/s10052-022-10182-7},
Key = {fds363185}
}
@article{fds356623,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for four-top-quark production in the single-lepton
and opposite-sign dilepton final states in pp collisions at
s =13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {99},
Number = {5},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.99.052009},
Abstract = {A search for four-top-quark production, tttt, is presented.
It is based on proton-proton collision data with a
center-of-mass energy s=13 TeV collected by the ATLAS
detector at the Large Hadron Collider during the years 2015
and 2016, corresponding to an integrated luminosity of 36.1
fb-1. Data are analyzed in both the single-lepton and
opposite-sign dilepton channels, characterized by the
presence of one or two isolated electrons or muons with
high-transverse momentum and multiple jets. A data-driven
method is used to estimate the dominant background from
top-quark pair production in association with jets. No
significant excess above the Standard Model expectation is
observed. The result is combined with the previous same-sign
dilepton and multilepton searches carried out by the ATLAS
Collaboration and an observed (expected) upper limit of 5.3
(2.1) times the four-top-quark Standard Model cross section
is obtained at 95% confidence level. Additionally, an upper
limit on the anomalous four-top-quark production cross
section is set in the context of an effective field theory
model.},
Doi = {10.1103/PhysRevD.99.052009},
Key = {fds356623}
}
@article{fds307951,
Author = {Aaltonen, T and others},
Title = {Search for Gluino-Mediated Bottom Squark Production in
p[overline p] Collisions at sqrt(s) = 1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {22},
Pages = {221801},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.221801},
Abstract = {We report on a search for the supersymmetric partner of the
bottom quark produced from gluino decays in data from 2.5
fb;{-1} of integrated luminosity collected by the Collider
Detector at Fermilab at sqrt[s]=1.96 TeV. Candidate events
are selected requiring two or more jets and large missing
transverse energy. At least two of the jets are required to
be tagged as originating from a b quark to enhance the
sensitivity. The results are in good agreement with the
prediction of the standard model processes, giving no
evidence for gluino decay to bottom squarks. This result
constrains the gluino-pair-production cross section to be
less than 40 fb at 95% credibility level for a gluino mass
of 350 GeV/c;{2}.},
Doi = {10.1103/physrevlett.102.221801},
Key = {fds307951}
}
@article{fds321084,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji,
W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin,
S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret,
MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini,
I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for gluinos in events with an isolated lepton, jets
and missing transverse momentum at [Formula: see text] = 13
Te V with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {565},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4397-x},
Abstract = {The results of a search for gluinos in final states with an
isolated electron or muon, multiple jets and large missing
transverse momentum using proton-proton collision data at a
centre-of-mass energy of [Formula: see text] are presented.
The dataset used was recorded in 2015 by the ATLAS
experiment at the Large Hadron Collider and corresponds to
an integrated luminosity of 3.2 fb[Formula: see text]. Six
signal selections are defined that best exploit the signal
characteristics. The data agree with the Standard Model
background expectation in all six signal selections, and the
largest deviation is a 2.1 standard deviation excess. The
results are interpreted in a simplified model where
pair-produced gluinos decay via the lightest chargino to the
lightest neutralino. In this model, gluinos are excluded up
to masses of approximately 1.6 Te V depending on the mass
spectrum of the simplified model, thus surpassing the limits
of previous searches.},
Doi = {10.1140/epjc/s10052-016-4397-x},
Key = {fds321084}
}
@article{fds307699,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth,
CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catinaccio, A and Catmore, JR and Cattai,
A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B},
Title = {Search for gluinos in events with two same-sign leptons,
jets, and missing transverse momentum with the ATLAS
detector in pp collisions at sqrt[s]=7 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {24},
Pages = {241802},
Year = {2012},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.108.241802},
Abstract = {A search is presented for gluinos decaying via the
supersymmetric partner of the top quark using events with
two same-sign leptons, jets, and missing transverse
momentum. The analysis is performed with 2.05 fb(-1) of
integrated luminosity from pp collisions at
sqrt[s]=7 TeV collected by the ATLAS detector at the
LHC. No excess beyond the standard model expectation is
observed, and exclusion limits are derived for simplified
models where the gluino decays via the supersymmetric
partner of the top quark and in the minimal supergravity and
constrained minimal supersymmetric standard model framework.
In those scenarios, gluino masses below 550 GeV are excluded
at 95% C.L. within the parameter space considered,
significantly extending the coverage with respect to
existing limits. Depending on the model parameters, gluino
masses up to 750 GeV can also be excluded at 95%
C.L.},
Doi = {10.1103/physrevlett.108.241802},
Key = {fds307699}
}
@article{fds307965,
Author = {Aaltonen, T and others},
Title = {Search for hadronic decays of W and Z bosons in photon
events in pp̅ collisions at sqrt[s] =1.96
TeV},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {5},
Pages = {052011},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.052011},
Abstract = {We report on a search for the process pp̅ →γ+W/Z with
W/Z→qq̅ in events containing two jets and a photon at the
center-of-mass energy sqrt[s]=1.96 TeV, using
184 pb-1 of data collected by the CDF II detector. A
neural network event selection has been developed to
optimize the rejection of the large QCD production
background; it is shown that this method gives a significant
improvement in both signal-to-noise ratio and signal
sensitivity, as compared with an event selection based on
conventional cuts. An upper limit is presented for the
γ+W/Z production cross section with the W and Z decaying
hadronically.},
Doi = {10.1103/PhysRevD.80.052011},
Key = {fds307965}
}
@article{fds347475,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Li, C-Q and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and CalventeLopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho
Toro, R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati,
L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Search for heavy ZZ resonances in the ℓ + ℓ - ℓ
+ ℓ - and ℓ + ℓ - ν ν ¯ final states using
proton-proton collisions at s = 13 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {4},
Pages = {293},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5686-3},
Abstract = {A search for heavy resonances decaying into a pair of Z
bosons leading to ℓ + ℓ - ℓ + ℓ - and ℓ + ℓ - ν
ν ¯ final states, where ℓ stands for either an electron
or a muon, is presented. The search uses proton-proton
collision data at a centre-of-mass energy of 13 TeV
corresponding to an integrated luminosity of 36.1 fb - 1
collected with the ATLAS detector during 2015 and 2016 at
the Large Hadron Collider. Different mass ranges for the
hypothetical resonances are considered, depending on the
final state and model. The different ranges span between 200
and 2000 GeV . The results are interpreted as upper limits
on the production cross section of a spin-0 or spin-2
resonance. The upper limits for the spin-0 resonance are
translated to exclusion contours in the context of Type-I
and Type-II two-Higgs-doublet models, while those for the
spin-2 resonance are used to constrain the Randall-Sundrum
model with an extra dimension giving rise to spin-2 graviton
excitations.},
Doi = {10.1140/epjc/s10052-018-5686-3},
Key = {fds347475}
}
@article{fds307850,
Author = {Aaltonen, and T, and al, E},
Title = {Search for Heavy Bottomlike Quarks Decaying to an Electron
or Muon and Jets in $p\overline{p}$ Collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {14},
Pages = {141803},
Publisher = {American Physical Society},
Year = {2011},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.141803},
Abstract = {We report the most sensitive direct search for pair
production of fourth-generation bottomlike chiral quarks
(b') each decaying promptly to tW. We search for an excess
of events with an electron or muon, at least five jets (one
identified as due to a b or c quark), and an imbalance of
transverse momentum by using data from pp collisions
collected by the CDF II detector at Fermilab with an
integrated luminosity of 4.8 fb(-1). We observe events
consistent with background expectation, calculate upper
limits on the b' pair-production cross section (σ(bb'))
≲30 fb for m(b') > 375 GeV/c2), and exclude
m(b') < 372 GeV/c2 at 95% confidence level assuming a
100% branching ratio of b' to tW.},
Doi = {10.1103/PhysRevLett.106.141803},
Key = {fds307850}
}
@article{fds348657,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Search for heavy charged long-lived particles in
proton–proton collisions at √s=13TeV using an ionisation
measurement with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {788},
Pages = {96-116},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2018.10.055},
Abstract = {This Letter presents a search for heavy charged long-lived
particles produced in proton–proton collisions at s=13TeV
at the LHC using a data sample corresponding to an
integrated luminosity of 36.1fb−1 collected by the ATLAS
experiment in 2015 and 2016. These particles are expected to
travel with a velocity significantly below the speed of
light, and therefore have a specific ionisation higher than
any high-momentum Standard Model particle of unit charge.
The pixel subsystem of the ATLAS detector is used in this
search to measure the ionisation energy loss of all
reconstructed charged particles which traverse the pixel
detector. Results are interpreted assuming the pair
production of R-hadrons as composite colourless states of a
long-lived gluino and Standard Model partons. No significant
deviation from Standard Model background expectations is
observed, and lifetime-dependent upper limits on R-hadron
production cross-sections and gluino masses are set,
assuming the gluino always decays to two quarks and a 100
GeV stable neutralino. R-hadrons with lifetimes above 1.0 ns
are excluded at the 95% confidence level, with lower limits
on the gluino mass ranging between 1290 GeV and 2060 GeV. In
the case of stable R-hadrons, the lower limit on the gluino
mass at the 95% confidence level is 1890
GeV.},
Doi = {10.1016/j.physletb.2018.10.055},
Key = {fds348657}
}
@article{fds356596,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA},
Title = {Search for heavy charged long-lived particles in the ATLAS
detector in 36.1 fb-1 of proton-proton collision data at s
=13 TeV},
Journal = {Physical Review D},
Volume = {99},
Number = {9},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.99.092007},
Abstract = {A search for heavy charged long-lived particles is performed
using a data sample of 36.1 fb-1 of proton-proton collisions
at s=13 TeV collected by the ATLAS experiment at the Large
Hadron Collider. The search is based on observables related
to ionization energy loss and time of flight, which are
sensitive to the velocity of heavy charged particles
traveling significantly slower than the speed of light.
Multiple search strategies for a wide range of lifetimes,
corresponding to path lengths of a few meters, are defined
as model independently as possible, by referencing several
representative physics cases that yield long-lived particles
within supersymmetric models, such as gluinos/squarks
(R-hadrons), charginos and staus. No significant deviations
from the expected Standard Model background are observed.
Upper limits at 95% confidence level are provided on the
production cross sections of long-lived R-hadrons as well as
directly pair-produced staus and charginos. These results
translate into lower limits on the masses of long-lived
gluino, sbottom and stop R-hadrons, as well as staus and
charginos of 2000, 1250, 1340, 430, and 1090 GeV,
respectively.},
Doi = {10.1103/PhysRevD.99.092007},
Key = {fds356596}
}
@article{fds354541,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche,
CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti,
C},
Title = {Search for heavy diboson resonances in semileptonic final
states in pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {12},
Publisher = {Springer Science and Business Media LLC},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08554-y},
Abstract = {This paper reports on a search for heavy resonances decaying
into WW, ZZ or WZ using proton–proton collision data at a
centre-of-mass energy of s=13 TeV. The data, corresponding
to an integrated luminosity of 139 fb 1, were recorded with
the ATLAS detector from 2015 to 2018 at the Large Hadron
Collider. The search is performed for final states in which
one W or Z boson decays leptonically, and the other W boson
or Z boson decays hadronically. The data are found to be
described well by expected backgrounds. Upper bounds on the
production cross sections of heavy scalar, vector or tensor
resonances are derived in the mass range 300–5000 GeV
within the context of Standard Model extensions with warped
extra dimensions or including a heavy vector triplet.
Production through gluon–gluon fusion, Drell–Yan or
vector-boson fusion are considered, depending on the assumed
model.},
Doi = {10.1140/epjc/s10052-020-08554-y},
Key = {fds354541}
}
@article{fds347487,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel,
M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C},
Title = {Search for Heavy Higgs Bosons A/H Decaying to a Top Quark
Pair in pp Collisions at sqrt[s]=8 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {119},
Number = {19},
Pages = {191803},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.119.191803},
Abstract = {A search for heavy pseudoscalar (A) and scalar (H) Higgs
bosons decaying into a top quark pair (tt[over ¯]) has been
performed with 20.3 fb^{-1} of proton-proton collision
data collected by the ATLAS experiment at the Large Hadron
Collider at a center-of-mass energy sqrt[s]=8 TeV.
Interference effects between the signal process and standard
model tt[over ¯] production, which are expected to distort
the signal shape from a single peak to a peak-dip structure,
are taken into account. No significant deviation from the
standard model prediction is observed in the tt[over ¯]
invariant mass spectrum in final states with an electron or
muon, large missing transverse momentum, and at least four
jets. The results are interpreted within the context of a
type-II two-Higgs-doublet model. Exclusion limits on the
signal strength are derived as a function of the mass
m_{A/H} and the ratio of the vacuum expectation values of
the two Higgs fields, tanβ, for m_{A/H}>500 GeV.},
Doi = {10.1103/physrevlett.119.191803},
Key = {fds347487}
}
@article{fds351557,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andrean, SY and Andreazza, A and Andrei,
V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Artz,
S and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou,
EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker,
OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour,
G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton,
AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso,
MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai,
P and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla,
JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borgna,
LS and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Bruncko,
D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buxo Vazquez,
CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero,
J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carney,
RMD and Caron, S and Carquin, E and Carrá, S and Carter, JWS and Carter,
TM and Casado, MP and Casha, AF and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavallaro, E and Cavasinni, V and Celebi,
E and Celli, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, YS and Christopher, LD and Chu, MC and Chu,
X and Chudoba, J and Chwastowski, JJ and Chytka, L and Cieri,
D},
Title = {Search for Heavy Higgs Bosons Decaying into Two Tau Leptons
with the ATLAS Detector Using pp Collisions at
sqrt[s]=13 TeV.},
Journal = {Physical review letters},
Volume = {125},
Number = {5},
Pages = {051801},
Year = {2020},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.125.051801},
Abstract = {A search for heavy neutral Higgs bosons is performed using
the LHC Run 2 data, corresponding to an integrated
luminosity of 139 fb^{-1} of proton-proton collisions
at sqrt[s]=13 TeV recorded with the ATLAS detector. The
search for heavy resonances is performed over the mass range
0.2-2.5 TeV for the τ^{+}τ^{-} decay with at least one
τ-lepton decaying into final states with hadrons. The data
are in good agreement with the background prediction of the
standard model. In the M_{h}^{125} scenario of the minimal
supersymmetric standard model, values of tanβ>8 and
tanβ>21 are excluded at the 95% confidence level for
neutral Higgs boson masses of 1.0 and 1.5 TeV,
respectively, where tanβ is the ratio of the vacuum
expectation values of the two Higgs doublets.},
Doi = {10.1103/physrevlett.125.051801},
Key = {fds351557}
}
@article{fds313595,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for heavy lepton resonances decaying to a Z boson and
a lepton in pp collisions at s√=8},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {9},
Pages = {1-38},
Publisher = {Springer Nature},
Year = {2015},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2015)108},
Abstract = {A search for heavy leptons decaying to a Z boson and an
electron or a muon is presented. The search is based on pp
collision data taken at (Formula presented.) = 8 TeV by the
ATLAS experiment at the CERN Large Hadron Collider,
corresponding to an integrated luminosity of 20.3 fb−1.
Three high-transverse-momentum electrons or muons are
selected, with two of them required to be consistent with
originating from a Z boson decay. No significant excess
above Standard Model background predictions is observed, and
95% confidence level limits on the production cross section
of high-mass trilepton resonances are derived. The results
are interpreted in the context of vector-like lepton and
type-III seesaw models. For the vector-like lepton model,
most heavy lepton mass values in the range 114–176 GeV are
excluded. For the type-III seesaw model, most mass values in
the range 100–468 GeV are excluded.},
Doi = {10.1007/JHEP09(2015)108},
Key = {fds313595}
}
@article{fds307865,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson,
KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov,
R and Ask, S},
Title = {Search for heavy long-lived charged particles with the ATLAS
detector in pp collisions at √s=7 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {703},
Number = {4},
Pages = {428-446},
Publisher = {Elsevier BV},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2011.08.042},
Abstract = {A search for long-lived charged particles reaching the muon
spectrometer is performed using a data sample of 37 pb-1
from pp collisions at √s=7 TeV collected by the ATLAS
detector at the LHC in 2010. No excess is observed above the
estimated background. Stable τ̃ sleptons are excluded at
95% CL up to a mass of 136 GeV, in GMSB models with N5=3,
mmessenger=250 TeV, sign(μ)=1 and tanβ=5. Electroweak
production of sleptons is excluded up to a mass of 110 GeV.
Gluino R-hadrons in a generic interaction model are excluded
up to masses of 530 GeV to 544 GeV depending on the fraction
of R-hadrons produced as g̃-balls. © 2011
CERN.},
Doi = {10.1016/j.physletb.2011.08.042},
Key = {fds307865}
}
@article{fds321088,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adersberger, M and Adomeit, S and Adye,
T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Search for heavy long-lived charged R-hadrons with the ATLAS
detector in 3.2 fb−1 of proton–proton
collision data at √s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {760},
Pages = {647-665},
Publisher = {Elsevier BV},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2016.07.042},
Abstract = {A search for heavy long-lived charged R-hadrons is reported
using a data sample corresponding to 3.2 fb−1 of
proton–proton collisions at s=13 TeV collected by the
ATLAS experiment at the Large Hadron Collider at CERN. The
search is based on observables related to large ionisation
losses and slow propagation velocities, which are signatures
of heavy charged particles travelling significantly slower
than the speed of light. No significant deviations from the
expected background are observed. Upper limits at 95%
confidence level are provided on the production cross
section of long-lived R-hadrons in the mass range from 600
GeV to 2000 GeV and gluino, bottom and top squark masses are
excluded up to 1580 GeV, 805 GeV and 890 GeV,
respectively.},
Doi = {10.1016/j.physletb.2016.07.042},
Key = {fds321088}
}
@article{fds310334,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
C},
Title = {Search for heavy long-lived multi-charged particles in
pp collisions at [Formula: see text] TeV using the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {8},
Pages = {362},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3534-2},
Abstract = {A search for heavy long-lived multi-charged particles is
performed using the ATLAS detector at the LHC. Data
collected in 2012 at [Formula: see text] TeV from <i>pp</i>
collisions corresponding to an integrated luminosity of
20.3 fb[Formula: see text]are examined. Particles producing
anomalously high ionisation, consistent with long-lived
massive particles with electric charges from [Formula: see
text] to [Formula: see text] are searched for. No signal
candidate events are observed, and 95 % confidence level
cross-section upper limits are interpreted as lower mass
limits for a Drell-Yan production model. The mass limits
range between 660 and 785 GeV.},
Doi = {10.1140/epjc/s10052-015-3534-2},
Key = {fds310334}
}
@article{fds375877,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos,
KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for heavy long-lived multi-charged particles in the
full LHC Run 2 pp collision data at s=13 TeV using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {847},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138316},
Abstract = {A search for heavy long-lived multi-charged particles is
performed using the ATLAS detector at the LHC. Data
collected in 2015–2018 at s=13 TeV from pp collisions
corresponding to an integrated luminosity of 139 fb−1 are
examined. Particles producing anomalously high ionization,
consistent with long-lived spin-½ massive particles with
electric charges from |q|=2e to |q|=7e are searched for. No
statistically significant evidence of such particles is
observed, and 95% confidence level cross-section upper
limits are calculated and interpreted as the lower mass
limits for a Drell–Yan plus photon-fusion production mode.
The least stringent limit, 1060 GeV, is obtained for |q|=2e
particles, and the most stringent one, 1600 GeV, is for
|q|=6e particles.},
Doi = {10.1016/j.physletb.2023.138316},
Key = {fds375877}
}
@article{fds356622,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA},
Title = {Search for heavy long-lived multicharged particles in
proton-proton collisions at s =13 TeV using the ATLAS
detector},
Journal = {Physical Review D},
Volume = {99},
Number = {5},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.99.052003},
Abstract = {A search for heavy long-lived multicharged particles is
performed using the ATLAS detector at the LHC. Data with an
integrated luminosity of 36.1 fb-1 collected in 2015 and
2016 from proton-proton collisions at s=13 TeV are examined.
Particles producing anomalously high ionization, consistent
with long-lived massive particles with electric charges from
|q|=2e to |q|=7e, are searched for. No events are observed,
and 95% confidence level cross-section upper limits are
interpreted as lower mass limits for a Drell-Yan production
model. Multicharged particles with masses between 50 and
980-1220 GeV (depending on their electric charge) are
excluded.},
Doi = {10.1103/PhysRevD.99.052003},
Key = {fds356622}
}
@article{fds316568,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold,
H},
Title = {Search for heavy Majorana neutrinos with the ATLAS detector
in pp collisions at √s = 8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {7},
Publisher = {Springer Nature},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2015)162},
Abstract = {Abstract: A search for heavy Majorana neutrinos in events
containing a pair of high-pT leptons of the same charge and
high-pT jets is presented. The search uses 20.3 fb−1 of pp
collision data collected with the ATLAS detector at the CERN
Large Hadron Collider with a centre-of-mass energy of 221as
= 8 TeV. The data are found to be consistent with the
background-only hypothesis based on the Standard Model
expectation. In the context of a Type-I seesaw mechanism,
limits are set on the production cross-section times
branching ratio for production of heavy Majorana neutrinos
in the mass range between 100 and 500 GeV. The limits are
subsequently interpreted as limits on the mixing between the
heavy Majorana neutrinos and the Standard Model neutrinos.
In the context of a left-right symmetric model, limits on
the production cross-section times branching ratio are set
with respect to the masses of heavy Majorana neutrinos and
heavy gauge bosons WR and Z′.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP07(2015)162},
Key = {fds316568}
}
@article{fds375849,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel,
A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed,
WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez,
AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Arcangeletti,
C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Tame,
ZPA and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten,
K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis, K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Gupta, DB and Balasubramanian, R and Baldin,
EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas,
WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits,
M-S and Barklow, T and Baron, P and Moreno, DAB and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Navarro, LB and Barreiro, F and da
Costa, JBG and Barron, U and Teixeira, MGB and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Hurrell, LTB and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Kuutmann, EB and Berger, N and Bergmann, B and Beringer, J and Bernardi,
G and Bernius, C and Bernlochner, FU and Bernon, F and Berry, T and Berta,
P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-sykes, CJ and Bird, GA and Birman, M and Biros, M and Bisanz, T and Bisceglie, E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Sola, JDB and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener,
R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and de Renstrom, PAB and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr, JTP and Burton,
CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Vazquez, CJB and Buzykaev, AR and Cabras, G and Urbán, SC and Caforio,
D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Toro, RC and Camarda, S and Munoz, DC and Camarri, P and Camerlingo, MT and Cameron,
D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Bret, MC and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Argos, FC and Carter, JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia,
EG and Castillo, FL and Garcia, LC and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli, A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen,
J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Moursli, RCE and Cheu, E and Cheung, K and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi,
K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron,
ZH},
Title = {Search for heavy Majorana or Dirac neutrinos and
right-handed W gauge bosons in final states with charged
leptons and jets in pp collisions at $$\sqrt{s}=13$$ TeV
with the ATLAS detector},
Journal = {The European Physical Journal C},
Volume = {83},
Number = {12},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {December},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-12021-9},
Abstract = {<jats:title>Abstract</jats:title><jats:p>A search for heavy
right-handed Majorana or Dirac neutrinos
<jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
and heavy right-handed gauge bosons <jats:inline-formula><jats:alternatives><jats:tex-math>$$W_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
is performed in events with energetic electrons or muons,
with the same or opposite electric charge, and energetic
jets. The search is carried out separately for topologies of
clearly separated final-state products (“resolved”
channel) and topologies with boosted final states with
hadronic and/or leptonic products partially overlapping and
reconstructed as a large-radius jet (“boosted” channel).
The events are selected from <jats:italic>pp</jats:italic>
collision data at the LHC with an integrated luminosity of
139 fb<jats:inline-formula><jats:alternatives><jats:tex-math>$$^{-1}$$</jats:tex-math>??
<mml:msup> <mml:mrow /> <mml:mrow> <mml:mo>-</mml:mo>
<mml:mn>1</mml:mn> </mml:mrow> </mml:msup>
</mml:math></jats:alternatives></jats:inline-formula>
collected by the ATLAS detector at <jats:inline-formula><jats:alternatives><jats:tex-math>$$\sqrt{s}
= 13$$</jats:tex-math>?? <mml:mrow> <mml:msqrt>
<mml:mi>s</mml:mi> </mml:msqrt> <mml:mo>=</mml:mo>
<mml:mn>13</mml:mn> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV.
No significant deviations from the Standard Model
predictions are observed. The results are interpreted within
the theoretical framework of a left-right symmetric model,
and lower limits are set on masses in the heavy right-handed
<jats:inline-formula><jats:alternatives><jats:tex-math>$$W_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
boson and <jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
plane. The excluded region extends to about
<jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})
= 6.4$$</jats:tex-math>?? <mml:mrow> <mml:mi>m</mml:mi>
<mml:mo>(</mml:mo> <mml:msub> <mml:mi>W</mml:mi>
<mml:mtext>R</mml:mtext> </mml:msub> <mml:mo>)</mml:mo>
<mml:mo>=</mml:mo> <mml:mn>6.4</mml:mn> </mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula> TeV
for both Majorana and Dirac <jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
neutrinos at <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(N_{\textrm{R}})<1$$</jats:tex-math>??
<mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
<mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
<mml:mo>)</mml:mo> <mml:mo><</mml:mo> <mml:mn>1</mml:mn>
</mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV.
<jats:inline-formula><jats:alternatives><jats:tex-math>$$N_{\textrm{R}}$$</jats:tex-math>??
<mml:msub> <mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext>
</mml:msub> </mml:math></jats:alternatives></jats:inline-formula>
with masses of less than 3.5 (3.6) TeV are excluded in the
electron (muon) channel at <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})=4.8$$</jats:tex-math>??
<mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
<mml:mi>W</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
<mml:mo>)</mml:mo> <mml:mo>=</mml:mo> <mml:mn>4.8</mml:mn>
</mml:mrow> </mml:math></jats:alternatives></jats:inline-formula> TeV
for the Majorana neutrinos, and limits of
<jats:inline-formula><jats:alternatives><jats:tex-math>$$m(N_{\textrm{R}})$$</jats:tex-math>??
<mml:mrow> <mml:mi>m</mml:mi> <mml:mo>(</mml:mo> <mml:msub>
<mml:mi>N</mml:mi> <mml:mtext>R</mml:mtext> </mml:msub>
<mml:mo>)</mml:mo> </mml:mrow> </mml:math></jats:alternatives></jats:inline-formula>
up to 3.6 TeV for <jats:inline-formula><jats:alternatives><jats:tex-math>$$m(W_{\textrm{R}})
= 5.2$$</jats:tex-math>?? <mml:mrow> <mml:mi>m</mml:mi>
<mml:mo>(</mml:mo> <mml:msub> <mml:mi>W</mml:mi>
<mml:mtext>R</mml:mtext> </mml:msub> <mml:mo>)</mml:mo>
<mml:mo>=</mml:mo> <mml:mn>5.2</mml:mn> </mml:mrow>
</mml:math></jats:alternatives></jats:inline-formula>
(5.0) TeV in the electron (muon) channel are set for the
Dirac neutrinos. These constitute the most stringent
exclusion limits to date for the model considered.</jats:p>},
Doi = {10.1140/epjc/s10052-023-12021-9},
Key = {fds375849}
}
@article{fds347450,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for heavy Majorana or Dirac neutrinos and
right-handed W gauge bosons in final states with two charged
leptons and two jets at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {1},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2019)016},
Abstract = {A search for heavy right-handed Majorana or Dirac neutrinos
NR and heavy right-handed gauge bosons WR is performed in
events with a pair of energetic electrons or muons, with the
same or opposite electric charge, and two energetic jets.
The events are selected from pp collision data with an
integrated luminosity of 36.1 fb−1 collected by the ATLAS
detector at s=13 TeV. No significant deviations from the
Standard Model are observed. The results are interpreted
within the theoretical framework of a left-right symmetric
model and lower limits are set on masses in the heavy
right-handed W boson and neutrino mass plane. The excluded
region extends to mRR=4.7 TeV for both Majorana and Dirac NR
neutrinos.},
Doi = {10.1007/JHEP01(2019)016},
Key = {fds347450}
}
@article{fds307804,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
Title = {Search for heavy metastable particles decaying to jet pairs
in pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012007},
Abstract = {A search is performed for heavy metastable particles that
decay into jet pairs with a macroscopic lifetime (cτ∼1cm)
in pp̄ collisions at √s=1.96TeV using data from the CDF
II detector at Fermilab corresponding to an integrated
luminosity of 3.2fb-1. To estimate the standard model
background, a data-driven approach is used.
Probability-density functions are constructed to model
secondary vertices from known processes. No statistically
significant excess is observed above the background. Limits
on the production cross section in a hidden valley benchmark
phenomenology are set for various Higgs boson masses as well
as metastable particle masses and lifetimes. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.012007},
Key = {fds307804}
}
@article{fds353483,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Search for heavy neutral Higgs bosons produced in
association with b-quarks and decaying into b-quarks at s
=13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {102},
Number = {3},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.102.032004},
Abstract = {A search for heavy neutral Higgs bosons produced in
association with one or two b-quarks and decaying to b-quark
pairs is presented using 27.8 fb-1 of s=13 TeV proton-proton
collision data recorded by the ATLAS detector at the Large
Hadron Collider during 2015 and 2016. No evidence of a
signal is found. Upper limits on the heavy neutral Higgs
boson production cross section times its branching ratio to
bb¯ are set, ranging from 4.0 to 0.6 pb at 95% confidence
level over a Higgs boson mass range of 450 to 1400 GeV.
Results are interpreted within the two-Higgs-doublet model
and the minimal supersymmetric Standard Model.},
Doi = {10.1103/PhysRevD.102.032004},
Key = {fds353483}
}
@article{fds356571,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz,
V},
Title = {Search for heavy neutral leptons in decays of W bosons
produced in 13 TeV pp collisions using prompt and displaced
signatures with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {10},
Year = {2019},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2019)265},
Abstract = {The problems of neutrino masses, matter-antimatter
asymmetry, and dark matter could be successfully addressed
by postulating right-handed neutrinos with Majorana masses
below the electroweak scale. In this work, leptonic decays
of W bosons extracted from 32.9 fb−1 to 36.1 fb−1 of 13
TeV proton–proton collisions at the LHC are used to search
for heavy neutral leptons (HNLs) that are produced through
mixing with muon or electron neutrinos. The search is
conducted using the ATLAS detector in both prompt and
displaced leptonic decay signatures. The prompt signature
requires three leptons produced at the interaction point
(either μμe or eeμ) with a veto on same-flavour
opposite-charge topologies. The displaced signature
comprises a prompt muon from the W boson decay and the
requirement of a dilepton vertex (either μμ or μe)
displaced in the transverse plane by 4–300 mm from the
interaction point. The search sets constraints on the HNL
mixing to muon and electron neutrinos for HNL masses in the
range 4.5–50 GeV. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2019)265},
Key = {fds356571}
}
@article{fds372388,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avner, G and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini,
G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker,
K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
Kuutmann, E and Berger, N and Bergmann, B and Beringer, J and Berlendis,
S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes,
CJ and Bird, GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde,
B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks,
WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko,
D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler,
JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez,
CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai, Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura,
P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet,
D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas,
JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casadei,
D and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement, C and Clissa, L and Coadou, Y and Cobal,
M},
Title = {Search for Heavy Neutral Leptons in Decays of W Bosons Using
a Dilepton Displaced Vertex in sqrt[s]=13 TeV pp
Collisions with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {6},
Pages = {061803},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.131.061803},
Abstract = {A search for a long-lived, heavy neutral lepton (N) in
139 fb^{-1} of sqrt[s]=13 TeV pp collision data
collected by the ATLAS detector at the Large Hadron Collider
is reported. The N is produced via W→Nμ or W→Ne and
decays into two charged leptons and a neutrino, forming a
displaced vertex. The N mass is used to discriminate between
signal and background. No signal is observed, and limits are
set on the squared mixing parameters of the N with the
left-handed neutrino states for the N mass range
3 GeV<m_{N}<15 GeV. For the first time, limits are
given for both single-flavor and multiflavor mixing
scenarios motivated by neutrino flavor oscillation results
for both the normal and inverted neutrino-mass
hierarchies.},
Doi = {10.1103/physrevlett.131.061803},
Key = {fds372388}
}
@article{fds307723,
Author = {The ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins,
M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B and Clement, C},
Title = {Search for heavy neutrinos and right-handed W bosons
in events with two leptons and jets in pp collisions
at [Formula: see text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {72},
Number = {7},
Pages = {2056},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2056-4},
Abstract = {This letter reports on a search for hypothetical heavy
neutrinos, <i>N</i>, and right-handed gauge bosons,
<i>W</i><sub>R</sub>, in events with high transverse
momentum objects which include two reconstructed leptons and
at least one hadronic jet. The results were obtained from
data corresponding to an integrated luminosity of
2.1 fb<sup>-1</sup> collected in proton-proton collisions
at [Formula: see text] with the ATLAS detector at the CERN
Large Hadron Collider. No excess above the Standard Model
background expectation is observed. Excluded mass regions
for Majorana and Dirac neutrinos are presented using two
approaches for interactions that violate lepton and
lepton-flavor numbers. One approach uses an effective
operator framework, the other approach is guided by the
Left-Right Symmetric Model. The results described in this
letter represent the most stringent limits to date on the
masses of heavy neutrinos and <i>W</i><sub>R</sub> bosons
obtained in direct searches.},
Doi = {10.1140/epjc/s10052-012-2056-4},
Key = {fds307723}
}
@article{fds356598,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA},
Title = {Search for heavy particles decaying into a top-quark pair in
the fully hadronic final state in pp collisions at s =13 TeV
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {99},
Number = {9},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.99.092004},
Abstract = {A search for new particles decaying into a pair of top
quarks is performed using proton-proton collision data
recorded with the ATLAS detector at the Large Hadron
Collider at a center-of-mass energy of s=13 TeV
corresponding to an integrated luminosity of 36.1 fb-1.
Events consistent with top-quark pair production and the
fully hadronic decay mode of the top quarks are selected by
requiring multiple high transverse momentum jets including
those containing b-hadrons. Two analysis techniques,
exploiting dedicated top-quark pair reconstruction in
different kinematic regimes, are used to optimize the search
sensitivity to new hypothetical particles over a wide mass
range. The invariant mass distribution of the two
reconstructed top-quark candidates is examined for resonant
production of new particles with various spins and decay
widths. No significant deviation from the Standard Model
prediction is observed and limits are set on the production
cross-section times branching fraction for new hypothetical
Z′ bosons, dark-matter mediators, Kaluza-Klein gravitons
and Kaluza-Klein gluons. By comparing with the predicted
production cross sections, the Z′ boson in the
topcolor-assisted-technicolor model is excluded for masses
up to 3.1-3.6 TeV, the dark-matter mediators in a simplified
framework are excluded in the mass ranges from 0.8 to 0.9
TeV and from 2.0 to 2.2 TeV, and the Kaluza-Klein gluon is
excluded for masses up to 3.4 TeV, depending on the decay
widths of the particles.},
Doi = {10.1103/PhysRevD.99.092004},
Key = {fds356598}
}
@article{fds310120,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev,
VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett,
JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del
Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
T and Feher, S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grünendahl, S and Gupta,
A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hildreth, MD and Hirosky,
R and Hobbs, JD and Hoeneisen, B and Huang, Y and Illingworth, R and Ito,
AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Kehoe, R and Kharchilava, A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov,
AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Leflat, A and Leggett, C and Lehner, F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AK and Madaras, RJ and Malyshev, VL and Manankov, V and Mao, HS and Marshall, T and Martin, MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McDonald, J and McMahon, T and Melanson, HL and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov, N and Mondal,
NK and Montgomery, HE and Moore, RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Nunnemann, T and O'Neil, D and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Raja, R and Rajagopalan,
S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Santoro, A and Sawyer,
L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder,
A and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van
Kooten, R and Varelas, N and Vertogradov, LS and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev, EG and Zylberstejn,
A},
Title = {Search for heavy particles decaying into electron-positron
pairs in pp collisions.},
Journal = {Physical review letters},
Volume = {87},
Number = {6},
Pages = {061802},
Year = {2001},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.87.061802},
Abstract = {We present results of searches for technirho (rho(T)),
techniomega (omega(T)), and Z' particles, using the decay
channels rho(T),omega(T),Z'-->e(+)e(-). The search is based
on 124.8 pb(-1) of data collected by the D0 detector at the
Fermilab Tevatron during 1992-1996. In the absence of a
signal, we set 95% C.L. upper limits on the cross sections
for the processes pp-->rho(T),omega(T),Z'-->e(+)e(-) as a
function of the mass of the decaying particle. For certain
model parameters, we exclude the existence of degenerate
rho(T) and omega(T) states with masses below about 200 GeV.
We exclude a Z' with mass below 670 GeV, assuming that it
has the same couplings to fermions as the Z
boson.},
Doi = {10.1103/physrevlett.87.061802},
Key = {fds310120}
}
@article{fds336450,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JSB and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, DC and Chan, SK and Chan,
WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, J and Chen, S and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard,
AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark, A},
Title = {Search for heavy particles decaying into top-quark pairs
using lepton-plus-jets events in proton-proton collisions at
s = 13 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {7},
Pages = {565},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5995-6},
Abstract = {A search for new heavy particles that decay into top-quark
pairs is performed using data collected from proton-proton
collisions at a centre-of-mass energy of 13 TeV by the
ATLAS detector at the Large Hadron Collider. The integrated
luminosity of the data sample is 36.1 fb - 1 . Events
consistent with top-quark pair production are selected by
requiring a single isolated charged lepton, missing
transverse momentum and jet activity compatible with a
hadronic top-quark decay. Jets identified as likely to
contain <i>b</i>-hadrons are required to reduce the
background from other Standard Model processes. The
invariant mass spectrum of the candidate top-quark pairs is
examined for local excesses above the background
expectation. No significant deviations from the Standard
Model predictions are found. Exclusion limits are set on the
production cross-section times branching ratio for
hypothetical Z ' bosons, Kaluza-Kein gluons and Kaluza-Klein
gravitons that decay into top-quark pairs.},
Doi = {10.1140/epjc/s10052-018-5995-6},
Key = {fds336450}
}
@booklet{Abbott98f,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Babukhadia, L and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and Del-Signore, K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Search for heavy pointlike dirac monopoles},
Journal = {Physical Review Letters},
Volume = {81},
Number = {3},
Pages = {524-529},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.81.524},
Abstract = {We have searched for central production of a pair of photons
with high transverse energies in pp̄ collisions at √s=1.8
TeV using 70pb-1 of data collected with the D0 detector at
the Fermilab Tevatron in 1994-1996. If they exist virtual
heavy pointlike Dirac monopoles could rescatter pairs of
nearly real photons into this final state via a box diagram.
We observe no excess of events above background and set
lower 95% C.L. limits of 610 870 or 1580 GeV/c2 on the mass
of a spin 0 1/2 or 1 Dirac monopole. © 1998 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.81.524},
Key = {Abbott98f}
}
@article{fds347463,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque,
JP and Araujo Ferraz and V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron,
S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn,
R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Colasurdo,
L},
Title = {Search for heavy resonances decaying into WW in the e
ν μ ν final state in pp collisions at s = 13 TeV
with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {1},
Pages = {24},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5491-4},
Abstract = {A search for neutral heavy resonances is performed in the W
W → e ν μ ν decay channel using <i>pp</i> collision
data corresponding to an integrated luminosity of 36.1 fb -
1 , collected at a centre-of-mass energy of 13 TeV by the
ATLAS detector at the Large Hadron Collider. No evidence of
such heavy resonances is found. In the search for production
via the quark-antiquark annihilation or gluon-gluon fusion
process, upper limits on σ X × B ( X → W W ) as a
function of the resonance mass are obtained in the mass
range between 200 GeV and up to 5 TeV for various benchmark
models: a Higgs-like scalar in different width scenarios, a
two-Higgs-doublet model, a heavy vector triplet model, and a
warped extra dimensions model. In the vector-boson fusion
process, constraints are also obtained on these resonances,
as well as on a Higgs boson in the Georgi-Machacek model and
a heavy tensor particle coupling only to gauge
bosons.},
Doi = {10.1140/epjc/s10052-017-5491-4},
Key = {fds347463}
}
@article{fds356047,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Search for heavy resonances decaying into a pair of Z bosons
in the ℓ+ℓ-ℓ′
+ℓ′ - and ℓ+ℓ-νν¯
final states using 139 fb - 1 of proton–proton
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09013-y},
Abstract = {A search for heavy resonances decaying into a pair of Z
bosons leading to ℓ+ℓ-ℓ′ +ℓ′ - and
ℓ+ℓ-νν¯ final states, where ℓ stands for either an
electron or a muon, is presented. The search uses
proton–proton collision data at a centre-of-mass energy of
13 TeV collected from 2015 to 2018 that corresponds to the
integrated luminosity of 139 fb - 1 recorded by the ATLAS
detector during Run 2 of the Large Hadron Collider.
Different mass ranges spanning 200 GeV to 2000 GeV for the
hypothetical resonances are considered, depending on the
final state and model. In the absence of a significant
observed excess, the results are interpreted as upper limits
on the production cross section of a spin-0 or spin-2
resonance. The upper limits for the spin-0 resonance are
translated to exclusion contours in the context of Type-I
and Type-II two-Higgs-doublet models, and the limits for the
spin-2 resonance are used to constrain the Randall–Sundrum
model with an extra dimension giving rise to spin-2 graviton
excitations.},
Doi = {10.1140/epjc/s10052-021-09013-y},
Key = {fds356047}
}
@article{fds355022,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling,
J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker,
OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Balli, F and Balunas,
WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett,
RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr,
AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa,
HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold,
A and Bertram, IA and Bessidskaia Bylund and O and Besson, N and Bethani,
A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya,
DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman, M and Bisanz, T and Biswal,
JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek,
T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden
Madden, WD and Brendlinger, K and Brener, R and Brenner, L and Brenner,
R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati,
L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carratta,
G and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Cavaliere, V and Cavasinni, V and Celebi, E and Celli, F and Cerny,
K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chatterjee, M and Chau, CC and Che, S and Chekanov,
S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen,
Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias,
TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ},
Title = {Search for Heavy Resonances Decaying into a Photon and a
Hadronically Decaying Higgs Boson in pp Collisions at
sqrt[s]=13 TeV with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {125},
Number = {25},
Pages = {251802},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.125.251802},
Abstract = {This Letter presents a search for the production of new
heavy resonances decaying into a Higgs boson and a photon
using proton-proton collision data at sqrt[s]=13 TeV
collected by the ATLAS detector at the LHC. The data
correspond to an integrated luminosity of 139 fb^{-1}.
The analysis is performed by reconstructing hadronically
decaying Higgs boson (H→bb[over ¯]) candidates as single
large-radius jets. A novel algorithm using information about
the jet constituents in the center-of-mass frame of the jet
is implemented to identify the two b quarks in the single
jet. No significant excess of events is observed above the
expected background. Upper limits are set on the production
cross-section times branching fraction for narrow spin-1
resonances decaying into a Higgs boson and a photon in the
resonance mass range from 0.7 to 4 TeV, cross-section times
branching fractions are excluded between 11.6 fb and
0.11 fb at a 95% confidence level.},
Doi = {10.1103/physrevlett.125.251802},
Key = {fds355022}
}
@article{fds336455,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for heavy resonances decaying into a W or Z boson and
a Higgs boson in final states with leptons and b-jets in 36
fb−1 of √s=13 TeV pp collisions with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {3},
Publisher = {Springer Nature},
Year = {2018},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2018)174},
Abstract = {A search is conducted for new resonances decaying into a W
or Z boson and a 125 GeV Higgs boson in the νν¯ bb¯ ,
ℓ±νbb¯ , and ℓ+ℓ−bb¯ final states, where ℓ± =
e± or μ±, in pp collisions at s=13 TeV. The data used
correspond to a total integrated luminosity of 36.1 fb−1
collected with the ATLAS detector at the Large Hadron
Collider during the 2015 and 2016 data-taking periods. The
search is conducted by examining the reconstructed invariant
or transverse mass distributions of W h and Zh candidates
for evidence of a localised excess in the mass range of 220
GeV up to 5 TeV. No significant excess is observed and the
results are interpreted in terms of constraints on the
production cross-section times branching fraction of heavy
W′ and Z′ resonances in heavy-vector-triplet models and
the CP-odd scalar boson A in two-Higgs-doublet models. Upper
limits are placed at the 95% confidence level and range
between 9.0 × 10−4 pb and 7.3 × 10−1 pb depending on
the model and mass of the resonance.[Figure not available:
see fulltext.].},
Doi = {10.1007/JHEP03(2018)174},
Key = {fds336455}
}
@article{fds356672,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for heavy resonances decaying to a photon and a
hadronically decaying Z /W /H boson in pp collisions at s
=13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {3},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.98.032015},
Abstract = {Many extensions of the Standard Model predict new resonances
decaying to a Z, W, or Higgs boson and a photon. This paper
presents a search for such resonances produced in pp
collisions at s=13 TeV using a data set with an integrated
luminosity of 36.1 fb-1 collected by the ATLAS detector at
the LHC. The Z/W/H bosons are identified through their
decays to hadrons. The data are found to be consistent with
the Standard Model expectation in the entire investigated
mass range. Upper limits are set on the production cross
section times branching fraction for resonance decays to
Z/W+γ in the mass range from 1.0 to 6.8 TeV and for the
first time into H+γ in the mass range from 1.0 to 3.0
TeV.},
Doi = {10.1103/PhysRevD.98.032015},
Key = {fds356672}
}
@article{fds356723,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Search for heavy resonances decaying to a W or Z boson and a
Higgs boson in the qq¯(′)bb¯ final state in
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {774},
Pages = {494-515},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2017.09.066},
Abstract = {A search for heavy resonances decaying to a W or Z boson and
a Higgs boson in the qq¯(′)bb¯ final state is described.
The search uses 36.1 fb−1 of proton–proton collision
data at s=13 TeV collected by the ATLAS detector at the CERN
Large Hadron Collider in 2015 and 2016. The data are in
agreement with the Standard Model expectations, with the
largest excess found at a resonance mass of 3.0 TeV with a
local (global) significance of 3.3 (2.1) σ. The results are
presented in terms of constraints on a simplified model with
a heavy vector triplet. Upper limits are set on the
production cross-section times branching ratio for
resonances decaying to a W (Z) boson and a Higgs boson,
itself decaying to bb¯, in the mass range between 1.1 and
3.8 TeV at 95% confidence level; the limits range between 83
and 1.6 fb (77 and 1.1 fb) at 95% confidence
level.},
Doi = {10.1016/j.physletb.2017.09.066},
Key = {fds356723}
}
@article{fds356765,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for heavy resonances decaying to a Z boson and a
photon in pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {764},
Pages = {11-30},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2016.11.005},
Abstract = {This Letter presents a search for new resonances with mass
larger than 250 GeV, decaying to a Z boson and a photon. The
dataset consists of an integrated luminosity of 3.2 fb−1
of pp collisions collected at s=13 TeV with the ATLAS
detector at the Large Hadron Collider. The Z bosons are
identified through their decays either to charged, light,
lepton pairs (e+e−, μ+μ−) or to hadrons. The data are
found to be consistent with the expected background in the
whole mass range investigated and upper limits are set on
the production cross section times decay branching ratio to
Zγ of a narrow scalar boson with mass between 250 GeV and
2.75 TeV.},
Doi = {10.1016/j.physletb.2016.11.005},
Key = {fds356765}
}
@article{fds307771,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and BenAmi, S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Böser, S and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik,
J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino,
G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya,
GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J},
Title = {Search for heavy vector-like quarks coupling to light quarks
in proton-proton collisions at √s=7 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {712},
Number = {1-2},
Pages = {22-39},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.03.082},
Abstract = {This Letter presents a search for singly produced
vector-like quarks, Q, coupling to light quarks, q. The
search is sensitive to both charged current (CC) and neutral
current (NC) processes, pp→Qq→Wqq' and pp→Qq→Zqq'
with a leptonic decay of the vector gauge boson. In 1.04fb-1
of data taken in 2011 by the ATLAS experiment at a
center-of-mass energy √s=7 TeV, no evidence of such heavy
vector-like quarks is observed above the expected Standard
Model background. Limits on the heavy vector-like quark
production cross section times branching ratio as a function
of mass mQ are obtained. For a coupling κqQ=v/mQ, where v
is the Higgs vacuum expectation value, 95% C.L. lower limits
on the mass of a vector-like quark are set at 900 GeV and
760 GeV from CC and NC processes, respectively. © 2012
CERN.},
Doi = {10.1016/j.physletb.2012.03.082},
Key = {fds307771}
}
@article{fds308053,
Author = {Abulencia, and A, and others},
Title = {Search for heavy, long-lived particles that decay to photons
at CDF II},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {12},
Pages = {121801},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.121801},
Abstract = {We present the first search for heavy, long-lived particles
that decay to photons at a hadron collider. We use a sample
of gamma+jet+missing transverse energy events in p[overline
p] collisions at sqrt(s)=1.96 TeV taken with the CDF II
detector. Candidate events are selected based on the arrival
time of the photon at the detector. Using an integrated
luminosity of 570 pb-1 of collision data, we observe 2
events, consistent with the background estimate of
1.3$\pm$0.7 events. While our search strategy does not rely
on model-specific dynamics, we set cross section limits in a
supersymmetric model with chi-tilde10-->gammaG-tilde and
place the world-best 95\% C.L. lower limit on the
chi-tilde10 mass of 101 GeV/c2 at tauchi-tilde[sub 1][sup
0]=5 ns.},
Doi = {10.1103/physrevlett.99.121801},
Key = {fds308053}
}
@article{fds375048,
Author = {A.V. Kotwal and the ATLAS Collaboration},
Title = {Search for heavy, long-lived, charged particles with large
ionisation energy loss in pp collisions at √s = 13 TeV
using the ATLAS experiment and the full Run 2
dataset},
Volume = {2023},
Number = {158},
Publisher = {Journal of High Energy Physics},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/https://doi.org/10.1007/JHEP06(2023)158},
Doi = {https://doi.org/10.1007/JHEP06(2023)158},
Key = {fds375048}
}
@article{fds310298,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
Title = {Search for Higgs and Z Boson Decays to J/ψγ and ϒ(nS)γ
with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {12},
Pages = {121801},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.114.121801},
Abstract = {A search for the decays of the Higgs and Z bosons to J/ψγ
and ϒ(nS)γ (n=1,2,3) is performed with pp collision data
samples corresponding to integrated luminosities of up to
20.3 fb^{-1} collected at sqrt[s]=8 TeV with the
ATLAS detector at the CERN Large Hadron Collider. No
significant excess of events is observed above expected
backgrounds and 95% C.L. upper limits are placed on the
branching fractions. In the J/ψγ final state the limits
are 1.5×10^{-3} and 2.6×10^{-6} for the Higgs and Z boson
decays, respectively, while in the ϒ(1S,2S,3S)γ final
states the limits are (1.3,1.9,1.3)×10^{-3} and
(3.4,6.5,5.4)×10^{-6}, respectively.},
Doi = {10.1103/physrevlett.114.121801},
Key = {fds310298}
}
@article{fds321089,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao De Mendizabal,
J and Billoud, TRV and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Search for Higgs and Z Boson Decays to ϕγ with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {117},
Number = {11},
Pages = {111802},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.117.111802},
Abstract = {A search for the decays of the Higgs and Z bosons to a ϕ
meson and a photon is performed with a pp collision data
sample corresponding to an integrated luminosity of
2.7 fb^{-1} collected at sqrt[s]=13 TeV with the
ATLAS detector at the LHC. No significant excess of events
is observed above the background, and 95% confidence level
upper limits on the branching fractions of the Higgs and Z
boson decays to ϕγ of 1.4×10^{-3} and 8.3×10^{-6},
respectively, are obtained.},
Doi = {10.1103/physrevlett.117.111802},
Key = {fds321089}
}
@article{fds356617,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for Higgs boson decays into a pair of light bosons in
the bbμμ final state in pp collision at √s=13TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {790},
Pages = {1-21},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2018.10.073},
Abstract = {A search for decays of the Higgs boson into a pair of new
spin-zero particles, H→aa, where the a-bosons decay into a
b-quark pair and a muon pair, is presented. The search uses
36.1 fb−1 of proton–proton collision data at s=13 TeV
recorded by the ATLAS experiment at the LHC in 2015 and
2016. No significant deviation from the Standard Model
prediction is observed. Upper limits at 95% confidence level
are placed on the branching ratio (σH/σSM)×B(H→aa→bbμμ),
ranging from 1.2×10−4 to 8.4×10−4 in the a-boson mass
range of 20–60 GeV. Model-independent limits are set on
the visible production cross-section times the branching
ratio to the bbμμ final state for new physics,
σvis(X)×B(X→bbμμ), ranging from 0.1 fb to 0.73 fb for
mμμ between 18 and 62 GeV.},
Doi = {10.1016/j.physletb.2018.10.073},
Key = {fds356617}
}
@article{fds354095,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling,
J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asai, K and Asai, S and Asawatavonvanich, T and Asbah, N and Asimakopoulou, EM and Asquith,
L and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Augsten, K and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Bachacou, H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani,
H and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker,
OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandieramonte, M and Bandyopadhyay, A and Banerjee, S and Barak,
L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bassalat, A and Basso, MJ and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Belfkir, M and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bhattacharya, DS and Bhattarai,
P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Biedermann,
D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Birman, M and Bisanz, T and Biswal, JP and Biswas,
D and Bitadze, A and Bittrich, C and Bjørke, K and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bogavac, D and Bogdanchikov,
AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Booth, CD and Borecka-Bielska, HM and Borgna, LS and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman
de Renstrom, PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
JTP and Burton, CD and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti,
P and Buttinger, W and Buxo Vazquez and CJ and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, F and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati,
L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carratta,
G and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castillo,
FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavallaro, E and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chadi, Z and Chakraborty, D and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christopher,
LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Chytka,
L},
Title = {Search for Higgs Boson Decays into a Z Boson and a Light
Hadronically Decaying Resonance Using 13 TeV pp Collision
Data from the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {125},
Number = {22},
Pages = {221802},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.125.221802},
Abstract = {A search for Higgs boson decays into a Z boson and a light
resonance in two-lepton plus jet events is performed, using
a pp collision dataset with an integrated luminosity of
139 fb^{-1} collected at sqrt[s]=13 TeV by the
ATLAS experiment at the CERN LHC. The resonance considered
is a light boson with a mass below 4 GeV from a possible
extended scalar sector or a charmonium state. Multivariate
discriminants are used for the event selection and for
evaluating the mass of the light resonance. No excess of
events above the expected background is found. Observed
(expected) 95% confidence-level upper limits are set on the
Higgs boson production cross section times branching
fraction to a Z boson and the signal resonance, with values
in the range 17-340 pb (16_{-5}^{+6}-320_{-90}^{+130} pb)
for the different light spin-0 boson mass and branching
fraction hypotheses, and with values of 110 and 100 pb
(100_{-30}^{+40} and 100_{-30}^{+40} pb) for the η_{c}
and J/ψ hypotheses, respectively.},
Doi = {10.1103/physrevlett.125.221802},
Key = {fds354095}
}
@article{fds356674,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for Higgs boson decays into pairs of light
(pseudo)scalar particles in the γγ jj final state in pp
collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {782},
Pages = {750-767},
Year = {2018},
Month = {July},
url = {http://dx.doi.org/10.1016/j.physletb.2018.06.011},
Abstract = {This Letter presents a search for exotic decays of the Higgs
boson to a pair of new (pseudo)scalar particles, H→aa,
where the a particle has a mass in the range 20–60 GeV,
and where one of the a bosons decays into a pair of photons
and the other to a pair of gluons. The search is performed
in event samples enhanced in vector-boson fusion Higgs boson
production by requiring two jets with large invariant mass
in addition to the Higgs boson candidate decay products. The
analysis is based on the full dataset of pp collisions at
s=13TeV recorded in 2015 and 2016 with the ATLAS detector at
the CERN Large Hadron Collider, corresponding to an
integrated luminosity of 36.7 fb−1. The data are in
agreement with the Standard Model predictions and an upper
limit at the 95% confidence level is placed on the
production cross section times the branching ratio for the
decay H→aa→γγgg. This limit ranges from 3.1 pb to 9.0
pb depending on the mass of the a boson.},
Doi = {10.1016/j.physletb.2018.06.011},
Key = {fds356674}
}
@article{fds356535,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk,
L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra,
JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo,
JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA},
Title = {Search for Higgs boson decays into two new low-mass spin-0
particles in the 4b channel with the ATLAS detector using pp
collisions at √s = 13 TeV},
Journal = {Physical Review D},
Volume = {102},
Number = {11},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.102.112006},
Abstract = {This paper describes a search for beyond the Standard Model
decays of the Higgs boson into a pair of new spin-0
particles subsequently decaying into b-quark pairs, H → aa
→ (bb¯)(bb¯), using protonproton collision data
collected by the ATLAS detector at the Large Hadron Collider
at center-of-mass energy √s = 13 TeV. This search focuses
on the range 15 GeV ≤ ma ≤ 30 GeV, where the decay
products are collimated; it is complementary to a previous
search in the same final state targeting the range 20 GeV
≤ ma ≤ 60 GeV, where the decay products are well
separated. A novel strategy for the identification of the a
→ bb¯ decays is deployed to enhance the efficiency for
topologies with small separation angles. The search is
performed with 36 fb-1 of integrated luminosity collected in
2015 and 2016 and sets upper limits on the production cross
section of H → aa → (bb¯)(bb¯), where the Higgs boson
is produced in association with a Z boson.},
Doi = {10.1103/PhysRevD.102.112006},
Key = {fds356535}
}
@article{fds307537,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and A°kesson, TPA and Akimoto, G and Akimov, AV and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Amidei, D and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ},
Title = {Search for Higgs boson decays to a photon and a Z boson in
pp collisions at s=7 and 8 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {732},
Pages = {8-27},
Publisher = {Elsevier BV},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2014.03.015},
Abstract = {A search is reported for a neutral Higgs boson in the decay
channel H→Zγ, Z→ℓ +ℓ -(ℓ = e, μ), using 4.5
fb-1of pp collisions at s=7 TeV and 20.3 fb-1of pp
collisions at s=8 TeV, recorded by the ATLAS detector at the
CERN Large Hadron Collider. The observed distribution of the
invariant mass of the three final-state particles,mℓℓγ,
is consistent with the Standard Model hypothesis in the
investigated mass range of 120-150 GeV. For a Higgs boson
with a mass of 125.5 GeV, the observed upper limit at the
95% confidence level is 11 times the Standard Model
expectation. Upper limits are set on the cross section times
branching ratio of a neutral Higgs boson with mass in the
range 120-150 GeV between 0.13 and 0.5 pb for s=8 TeV at 95%
confidence level. © 2014.},
Doi = {10.1016/j.physletb.2014.03.015},
Key = {fds307537}
}
@article{fds336453,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for Higgs boson decays to beyond-the-Standard-Model
light bosons in four-lepton events with the ATLAS detector
at √s=13 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {6},
Publisher = {Springer Nature},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2018)166},
Abstract = {A search is conducted for a beyond-the-Standard-Model boson
using events where a Higgs boson with mass 125 GeV decays to
four leptons (ℓ = e or μ). This decay is presumed to
occur via an intermediate state which contains one or two
on-shell, promptly decaying bosons: H → ZX/XX → 4ℓ,
where X is a new vector boson Zd or pseudoscalar a with mass
between 1 and 60 GeV. The search uses pp collision data
collected with the ATLAS detector at the LHC with an
integrated luminosity of 36.1 fb−1 at a centre-of-mass
energy s=13 TeV. No significant excess of events above
Standard Model background predictions is observed;
therefore, upper limits at 95% confidence level are set on
modelindependent fiducial cross-sections, and on the Higgs
boson decay branching ratios to vector and pseudoscalar
bosons in two benchmark models.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP06(2018)166},
Key = {fds336453}
}
@article{fds371449,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi,
MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for Higgs boson pair production in association with a
vector boson in pp collisions at √s=13TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11559-y},
Abstract = {This paper reports a search for Higgs boson pair (hh)
production in association with a vector boson (WorZ) using
139 fb - 1 of proton–proton collision data at s=13TeV
recorded with the ATLAS detector at the Large Hadron
Collider. The search is performed in final states in which
the vector boson decays leptonically (W→ℓν,Z→ℓℓ,νν
with ℓ= e, μ) and the Higgs bosons each decay into a pair
of b-quarks. It targets Vhh signals from both non-resonant
hh production, present in the Standard Model (SM), and
resonant hh production, as predicted in some SM extensions.
A 95% confidence-level upper limit of 183 (87) times the SM
cross-section is observed (expected) for non-resonant Vhh
production when assuming the kinematics are as expected in
the SM. Constraints are also placed on Higgs boson coupling
modifiers. For the resonant search, upper limits on the
production cross-sections are derived for two specific
models: one is the production of a vector boson along with a
neutral heavy scalar resonance H, in the mass range
260–1000 GeV, that decays into hh, and the other is the
production of a heavier neutral pseudoscalar resonance A
that decays into a Z boson and H boson, where the A boson
mass is 360–800 GeV and the H boson mass is
260–400 GeV. Constraints are also derived in the
parameter space of two-Higgs-doublet models.},
Doi = {10.1140/epjc/s10052-023-11559-y},
Key = {fds371449}
}
@article{fds356615,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S},
Title = {Search for Higgs boson pair production in the bb¯ WW
* decay mode at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {4},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2019)092},
Abstract = {A search for Higgs boson pair production in the bb¯ WW *
decay mode is performed in the bb¯ ℓνqq final state
using 36.1 fb −1 of proton-proton collision data at a
centre-of-mass energy of 13 TeV recorded with the ATLAS
detector at the Large Hadron Collider. No evidence of events
beyond the background expectation is found. Upper limits on
the non-resonant pp → HH production cross section of 10 pb
and on the resonant production cross section as a function
of the HH invariant mass are obtained. Resonant production
limits are set for scalar and spin-2 graviton hypotheses in
the mass range 500 to 3000 GeV.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP04(2019)092},
Key = {fds356615}
}
@article{fds356606,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Search for Higgs boson pair production in the
WW(*)WW(*) decay channel using ATLAS
data recorded at √s = 13 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2019)124},
Abstract = {A search for a pair of neutral, scalar bosons with each
decaying into two W bosons is presented using 36.1 fb−1 of
proton-proton collision data at a centre-of-mass energy of
13 TeV recorded with the ATLAS detector at the Large Hadron
Collider. This search uses three production models:
non-resonant and resonant Higgs boson pair production and
resonant production of a pair of heavy scalar particles.
Three final states, classified by the number of leptons, are
analysed: two same-sign leptons, three leptons, and four
leptons. No significant excess over the expected Standard
Model backgrounds is observed. An observed (expected) 95%
confidence-level upper limit of 160 (120) times the Standard
Model prediction of non-resonant Higgs boson pair production
cross-section is set from a combined analysis of the three
final states. Upper limits are set on the production
cross-section times branching ratio of a heavy scalar X
decaying into a Higgs boson pair in the mass range of 260
GeV ≤ mX ≤ 500 GeV and the observed (expected) limits
range from 9.3 (10) pb to 2.8 (2.6) pb. Upper limits are set
on the production cross-section times branching ratio of a
heavy scalar X decaying into a pair of heavy scalars S for
mass ranges of 280 GeV ≤ mX ≤ 340 GeV and 135 GeV ≤ mS
≤ 165 GeV and the observed (expected) limits range from
2.5 (2.5) pb to 0.16 (0.17) pb.},
Doi = {10.1007/JHEP05(2019)124},
Key = {fds356606}
}
@article{fds321139,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH},
Title = {Search for Higgs boson pair production in the [Formula: see
text] final state from pp collisions at [Formula: see
text] TeVwith the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {9},
Pages = {412},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3628-x},
Abstract = {A search for Higgs boson pair production [Formula: see text]
is performed with 19.5 fb[Formula: see text] of
proton-proton collision data at [Formula: see text] TeV,
which were recorded by the ATLAS detector at the Large
Hadron Collider in 2012. The decay products of each Higgs
boson are reconstructed as a high-momentum [Formula: see
text] system with either a pair of small-radius jets or a
single large-radius jet, the latter exploiting jet
substructure techniques and associated <i>b</i>-tagged
track-jets. No evidence for resonant or non-resonant Higgs
boson pair production is observed. The data are interpreted
in the context of the Randall-Sundrum model with a warped
extra dimension as well as the two-Higgs-doublet model. An
upper limit on the cross-section for [Formula: see text] of
3.2 (2.3) fb is set for a Kaluza-Klein graviton [Formula:
see text] mass of 1.0 (1.5) TeV, at the 95 % confidence
level. The search for non-resonant Standard Model <i>hh</i>
production sets an observed 95 % confidence level upper
limit on the production cross-section [Formula: see text] of
202 fb, compared to a Standard Model prediction of
[Formula: see text] fb.},
Doi = {10.1140/epjc/s10052-015-3628-x},
Key = {fds321139}
}
@article{fds356647,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for Higgs boson pair production in the γ γ bb¯
final state with 13 TeV pp collision data collected by the
ATLAS experiment},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {11},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2018)040},
Abstract = {A search is performed for resonant and non-resonant Higgs
boson pair production in the γ γ bb¯ final state. The
data set used corresponds to an integrated luminosity of
36.1 fb−1 of proton-proton collisions at a centre-of-mass
energy of 13 TeV recorded by the ATLAS detector at the CERN
Large Hadron Collider. No significant excess relative to the
Standard Model expectation is observed. The observed limit
on the non-resonant Higgs boson pair cross-section is 0.73
pb at 95% confidence level. This observed limit is
equivalent to 22 times the predicted Standard Model
cross-section. The Higgs boson self-coupling (κλ =
λHHH/λHHHSM) is constrained at 95% confidence level to
−8.2 < κλ < 13.2. For resonant Higgs boson pair
production through X→ HH→ γ γ bb¯ , the limit is
presented, using the narrow-width approximation, as a
function of mX in the range 260 GeV < mX < 1000 GeV. The
observed limits range from 1.1 pb to 0.12 pb over this mass
range.},
Doi = {10.1007/JHEP11(2018)040},
Key = {fds356647}
}
@article{fds347486,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines,
JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen,
S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng,
HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ},
Title = {Search for Higgs boson pair production in the γ γ W W ∗
channel using pp collision data recorded at s = 13 TeV with
the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {12},
Pages = {1007},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6457-x},
Abstract = {Searches for non-resonant and resonant Higgs boson pair
production are performed in the γ γ W W ∗ channel with
the final state of γ γ ℓ ν j j using 36.1 fb - 1 of
proton-proton collision data recorded at a centre-of-mass
energy of s = 13 TeV by the ATLAS detector at the Large
Hadron Collider. No significant deviation from the Standard
Model prediction is observed. A 95% confidence-level
observed upper limit of 7.7 pb is set on the cross section
for non-resonant production, while the expected limit is 5.4
pb. A search for a narrow-width resonance <i>X</i> decaying
to a pair of Standard Model Higgs bosons <i>HH</i> is
performed with the same set of data, and the observed upper
limits on σ ( p p → X ) × B ( X → H H ) range between
40.0 and 6.1 pb for masses of the resonance between 260 and
500 GeV, while the expected limits range between 17.6 and
4.4 pb. When deriving the limits above, the Standard Model
branching ratios of the H → γ γ and H → W W ∗ are
assumed.},
Doi = {10.1140/epjc/s10052-018-6457-x},
Key = {fds347486}
}
@article{fds310302,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, M and Battistin,
M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, MF and Besson, N and Betancourt,
C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea,
V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov,
A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet,
S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG},
Title = {Search for Higgs boson pair production in the γγbb[over
¯] final state using pp collision data at
sqrt[s]=8 TeV from the ATLAS detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {8},
Pages = {081802},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.114.081802},
Abstract = {Searches are performed for resonant and nonresonant Higgs
boson pair production in the γγbb[over ¯] final state
using 20 fb^{-1} of proton-proton collisions at a
center-of-mass energy of 8 TeV recorded with the ATLAS
detector at the CERN Large Hadron Collider. A 95% confidence
level upper limit on the cross section times branching ratio
of nonresonant production is set at 2.2 pb, while the
expected limit is 1.0 pb. The difference derives from a
modest excess of events, corresponding to 2.4 standard
deviations from the background-only hypothesis. The limit
observed in the search for a narrow X→hh resonance ranges
between 0.7 and 3.5 pb as a function of the resonance
mass.},
Doi = {10.1103/physrevlett.114.081802},
Key = {fds310302}
}
@article{fds355955,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin,
JF},
Title = {Search for Higgs boson production in association with a
high-energy photon via vector-boson fusion with decay into
bottom quark pairs at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {3},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2021)268},
Abstract = {A search is presented for the production of the Standard
Model Higgs boson in association with a high-energy photon.
With a focus on the vector-boson fusion process and the
dominant Higgs boson decay into b-quark pairs, the search
benefits from a large reduction of multijet background
compared to more inclusive searches. Results are reported
from the analysis of 132 fb−1 of pp collision data at s =
13 TeV collected with the ATLAS detector at the LHC. The
measured Higgs boson signal yield in this final-state
signature is 1.3 ± 1.0 times the Standard Model prediction.
The observed significance of the Higgs boson signal above
the background is 1.3 standard deviations, compared to an
expected significance of 1.0 standard deviations. [Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP03(2021)268},
Key = {fds355955}
}
@article{fds362571,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C},
Title = {Search for Higgs bosons decaying into new spin-0 or spin-1
particles in four-lepton final states with the ATLAS
detector with 139 fb −1 of pp collision data at
√s = 13 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2022},
Number = {3},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2022)041},
Abstract = {Searches are conducted for new spin-0 or spin-1 bosons using
events where a Higgs boson with mass 125 GeV decays into
four leptons (ℓ = e, μ). This decay is presumed to occur
via an intermediate state which contains two on-shell,
promptly decaying bosons: H → XX/ZX → 4ℓ, where the
new boson X has a mass between 1 and 60 GeV. The search uses
pp collision data collected with the ATLAS detector at the
LHC with an integrated luminosity of 139 fb−1 at a
centre-of-mass energy s = 13 TeV. The data are found to be
consistent with Standard Model expectations. Limits are set
on fiducial cross sections and on the branching ratio of the
Higgs boson to decay into XX/ZX, improving those from
previous publications by a factor between two and four.
Limits are also set on mixing parameters relevant in
extensions of the Standard Model containing a dark sector
where X is interpreted to be a dark boson. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP03(2022)041},
Key = {fds362571}
}
@article{fds321136,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and T. H.
Arce and A and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for higgs bosons decaying to aa in the µµττ final
state in pp collisions at √s = 8 TeV with the ATLAS
experiment},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {5},
Pages = {052002-1-052002-24},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.92.052002},
Abstract = {A search for the decay to a pair of new particles of either
the 125 GeV Higgs boson (h) or a second charge parity
(CP)-even Higgs boson (H) is presented. The data set
corresponds to an integrated luminosity of 20.3 fb-1 of pp
collisions at √s = 8 TeV recorded by the ATLAS experiment
at the LHC in 2012. The search was done in the context of
the next-to-minimal supersymmetric standard model, in which
the new particles are the lightest neutral pseudoscalar
Higgs bosons (a). One of the two a bosons is required to
decay to two muons while the other is required to decay to
two τ leptons. No significant excess is observed above the
expected backgrounds in the dimuon invariant mass range from
3.7 to 50 GeV. Upper limits are placed on the production of
h → aa relative to the standard model gg → h production,
assuming no coupling of the a boson to quarks. The most
stringent limit is placed at 3.5% for ma = 3.75 GeV. Upper
limits are also placed on the production cross section of H
→ aa from 2.33 to 0.72 pb, for fixed ma = 5 GeV with mH
ranging from 100 to 500 GeV.},
Doi = {10.1103/PhysRevD.92.052002},
Key = {fds321136}
}
@article{fds308101,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and DaRonco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann, JR and DiTuro,
P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Garcia Sciverez and M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and di
Giovanni, GP and Giannetti, P and Gibson, A and Gibson, K and Ginsburg,
C and Giokaris, N and Giolo, K and Giordani, M and Giunta, M and Giurgiu,
G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos,
K and Gresele, A and Griffiths, M and Grinstein, S and Grosso-Pilcher,
C and Grundler, U and Guimaraes da Costa and J and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris,
RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer,
A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang,
D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel,
M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong, DJ and Konigsberg, J and Kordas, K and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen,
AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and LeCompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis, JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss, TM and Lister, A and Litvintsev,
DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and MacQueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca,
G and Margaroli, F and Marginean, R and Marino, C and Martin, A and Martin,
M and Martin, V and Martínez, M and Maruyama, T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina,
A and von der Mey, M and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr,
B and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa,
T and Oh, SH and Oh, YD and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra,
J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot,
J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman,
A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and van Remortel, N and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori, L and Robertson,
WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov, A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle,
T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria,
F},
Title = {Search for Higgs bosons decaying to bb and produced in
association with W bosons in pp collisions at square root of
s = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {96},
Number = {8},
Pages = {081803},
Year = {2006},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.96.081803},
Abstract = {We present a search for Higgs bosons decaying into bb and
produced in association with W bosons in pp collisions at
square root of s = 1.96 TeV. This search uses 320 pb(-1) of
the data set accumulated by the upgraded Collider Detector
at Fermilab. Events are selected that have a high-transverse
momentum electron or muon, missing transverse energy, and
two jets, at least one of which is consistent with the
hadronization of a b quark. Both the number of events and
the dijet mass distribution are consistent with standard
model background expectations, and we set 95% confidence
level upper limits on the production cross section times
branching ratio for the Higgs boson or any new particle with
similar decay kinematics. These upper limits range from 10
pb for mH = 110 GeV/c2 to 3 pb for mH = 150
GeV/c2.},
Doi = {10.1103/physrevlett.96.081803},
Key = {fds308101}
}
@article{fds307937,
Author = {Aaltonen, T and others},
Title = {Search for Higgs Bosons Predicted in Two-Higgs-Doublet
Models via Decays to Tau Lepton Pairs in 1.96 TeV pp̅
Collisions},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {20},
Pages = {201801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.201801},
Abstract = {We present the results of a search for Higgs bosons
predicted in two-Higgs-doublet models, in the case where the
Higgs bosons decay to tau lepton pairs, using 1.8 fb-1
of integrated luminosity of pp̅ collisions recorded by the
CDF II experiment at the Fermilab Tevatron. Studying the
mass distribution in events where one or both tau leptons
decay leptonically, no evidence for a Higgs boson signal is
observed. The result is used to infer exclusion limits in
the two-dimensional space of tanβ versus mA (the ratio
of the vacuum expectation values of the two Higgs doublets
and the mass of the pseudoscalar boson, respectively).},
Doi = {10.1103/physrevlett.103.201801},
Key = {fds307937}
}
@article{fds307815,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Dagenhart, D},
Title = {Search for Higgs bosons produced in association with b
quarks},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.85.032005},
Abstract = {We present a search for neutral Higgs bosons decaying into
bb̄, produced in association with b quarks in pp̄
collisions. This process could be observable in
supersymmetric models with high values of tanβ. The event
sample corresponds to 2.6fb -1 of integrated luminosity
collected with the CDF II detector at the Fermilab Tevatron
collider. We search for an enhancement in the mass of the
two leading jets in events with three jets identified as
coming from b quarks using a displaced vertex algorithm. A
data-driven procedure is used to estimate the dijet mass
spectrum of the nonresonant multijet background. The
contributions of backgrounds and a possible Higgs boson
signal are determined by a two-dimensional fit of the data,
using the dijet mass together with an additional variable
which is sensitive to the flavor composition of the three
tagged jets. We set mass-dependent limits on
σ(pp̄→)×B(→bb̄) which are applicable for a narrow
scalar particle produced in association with b quarks. We
also set limits on tanβ in supersymmetric Higgs models
including the effects of the Higgs boson width. © 2012
American Physical Society.},
Doi = {10.1103/PhysRevD.85.032005},
Key = {fds307815}
}
@article{fds356663,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for Higgs bosons produced via vector-boson fusion and
decaying into bottom quark pairs in s =13 TeV pp collisions
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {5},
Year = {2018},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.98.052003},
Abstract = {A search for the bb decay of the Standard Model Higgs boson
produced through vector-boson fusion is presented. Three
mutually exclusive channels are considered: two all-hadronic
channels and a photon-associated channel. Results are
reported from the analysis of up to 30.6 fb-1 of pp data at
s=13 TeV collected with the ATLAS detector at the LHC. The
measured signal strength relative to the Standard Model
prediction from the combined analysis is 2.5-1.3+1.4 for
inclusive Higgs boson production and 3.0-1.6+1.7 for
vector-boson fusion production only.},
Doi = {10.1103/PhysRevD.98.052003},
Key = {fds356663}
}
@article{fds356619,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Search for Higgs-like particles produced in association with
bottom quarks in proton-antiproton collisions},
Journal = {Physical Review D},
Volume = {99},
Number = {5},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.99.052001},
Abstract = {We report on a search for a spin-zero non-standard model
particle in proton-antiproton collisions collected by the
Collider Detector at Fermilab at a center-of-mass-energy of
1.96 TeV. This particle, the φ boson, is expected to decay
into a bottom-antibottom quark pair and to be produced in
association with at least one bottom quark. The data sample
consists of events with three jets identified as initiated
by bottom quarks and corresponds to 5.4 fb-1 of integrated
luminosity. In each event, the invariant mass of the two
most energetic jets is studied by looking for deviations
from the multijet background, which is modeled using data.
No evidence is found for such a particle. Exclusion upper
limits ranging from 20 to 2 pb are set for the product of
production cross sections times branching fraction for the
hypothetical φ boson with mass between 100 and 300 GeV/c2.
These are the most stringent constraints to
date.},
Doi = {10.1103/PhysRevD.99.052001},
Key = {fds356619}
}
@article{fds307867,
Author = {Collaboration, AVKWGAEAATLAS},
Title = {Search for high mass dilepton resonances in pp collisions at
7 TeV with the ATLAS experiment},
Journal = {Physics Letters B},
Volume = {700},
Number = {3-4},
Pages = {163-180},
Publisher = {Elsevier BV},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1016/j.physletb.2011.04.044},
Abstract = {This Letter presents a search for high mass e+e- or μ+μ-
resonances in pp collisions at √s=7 TeV at the LHC. The
data were recorded by the ATLAS experiment during 2010 and
correspond to a total integrated luminosity of ~40 pb-1. No
statistically significant excess above the Standard Model
expectation is observed in the search region of dilepton
invariant mass above 110 GeV. Upper limits at the 95%
confidence level are set on the cross section times
branching ratio of Z' resonances decaying to dielectrons and
dimuons as a function of the resonance mass. A lower mass
limit of 1.048 TeV on the Sequential Standard Model Z' boson
is derived, as well as mass limits on Z* and E6-motivated Z'
models. © 2011 CERN.},
Doi = {10.1016/j.physletb.2011.04.044},
Key = {fds307867}
}
@article{fds307853,
Author = {Collaboration, AVKWTAEACDF},
Title = {Search for High Mass Resonances Decaying to Muon Pairs in
√s=1.96 TeV pp̅ Collisions},
Journal = {Physical Review Letters},
Volume = {106},
Number = {121801},
Pages = {7},
Publisher = {American Physical Society},
Year = {2011},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.121801},
Abstract = {We present a search for a new narrow, spin-1, high mass
resonance decaying to μ(+)μ⁻+X, using a
matrix-element-based likelihood and a simultaneous
measurement of the resonance mass and production rate. In
data with 4.6 fb⁻¹ of integrated luminosity collected by
the CDF detector in pp collisions at √s=1960 GeV, the most
likely signal cross section is consistent with zero at 16%
confidence level. We therefore do not observe evidence for a
high mass resonance and place limits on models predicting
spin-1 resonances, including M>1071 GeV/c² at 95%
confidence level for a Z' boson with the same couplings to
fermions as the Z boson.},
Doi = {10.1103/PhysRevLett.106.121801},
Key = {fds307853}
}
@article{fds313612,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for high-mass diboson resonances with boson-tagged
jets in proton-proton collisions at √s = 8TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {12},
Pages = {1-39},
Publisher = {Springer Nature},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2015)055},
Abstract = {Abstract: A search is performed for narrow resonances
decaying into WW, WZ, or ZZ boson pairs using 20.3 fb−1 of
proton-proton collision data at a centre-of-mass energy of
s=8$$ \sqrt{s}=8 $$ TeV recorded with the ATLAS detector at
the Large Hadron Collider. Diboson resonances with masses in
the range from 1.3 to 3.0 TeV are sought after using the
invariant mass distribution of dijets where both jets are
tagged as a boson jet, compatible with a highly boosted W or
Z boson decaying to quarks, using jet mass and substructure
properties. The largest deviation from a smoothly falling
background in the observed dijet invariant mass distribution
occurs around 2 TeV in the WZ channel, with a global
significance of 2.5 standard deviations. Exclusion limits at
the 95% confidence level are set on the production cross
section times branching ratio for the WZ final state of a
new heavy gauge boson, W′, and for the WW and ZZ final
states of Kaluza-Klein excitations of the graviton in a bulk
Randall-Sundrum model, as a function of the resonance mass.
W′ bosons with couplings predicted by the extended gauge
model in the mass range from 1.3 to 1.5 TeV are excluded at
95% confidence level.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP12(2015)055},
Key = {fds313612}
}
@article{fds310363,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allen, K and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Search for high-mass dilepton resonances in pp collisions at
s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052005},
Abstract = {The ATLAS detector at the Large Hadron Collider is used to
search for high-mass resonances decaying to dielectron or
dimuon final states. Results are presented from an analysis
of proton-proton (pp) collisions at a center-of-mass energy
of 8 TeV corresponding to an integrated luminosity of 20.3
fb-1 in the dimuon channel. A narrow resonance with Standard
Model Z couplings to fermions is excluded at 95% confidence
level for masses less than 2.79 TeV in the dielectron
channel, 2.53 TeV in the dimuon channel, and 2.90 TeV in the
two channels combined. Limits on other model interpretations
are also presented, including a grand-unification model
based on the E6 gauge group, Z∗ bosons, minimal Z′
models, a spin-2 graviton excitation from Randall-Sundrum
models, quantum black holes, and a minimal walking
technicolor model with a composite Higgs
boson.},
Doi = {10.1103/PhysRevD.90.052005},
Key = {fds310363}
}
@article{fds356575,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP},
Title = {Search for high-mass dilepton resonances using 139
fb−1 of pp collision data collected at √s=13
TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {796},
Pages = {68-87},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2019.07.016},
Abstract = {A search for high-mass dielectron and dimuon resonances in
the mass range of 250 GeV to 6 TeV is presented. The data
were recorded by the ATLAS experiment in proton–proton
collisions at a centre-of-mass energy of s=13 TeV during Run
2 of the Large Hadron Collider and correspond to an
integrated luminosity of 139 fb−1. A functional form is
fitted to the dilepton invariant-mass distribution to model
the contribution from background processes, and a generic
signal shape is used to determine the significance of
observed deviations from this background estimate. No
significant deviation is observed and upper limits are
placed at the 95% confidence level on the fiducial
cross-section times branching ratio for various resonance
width hypotheses. The derived limits are shown to be
applicable to spin-0, spin-1 and spin-2 signal hypotheses.
For a set of benchmark models, the limits are converted into
lower limits on the resonance mass and reach 4.5 TeV for the
E6-motivated Zψ′ boson. Also presented are limits on
Heavy Vector Triplet model couplings.},
Doi = {10.1016/j.physletb.2019.07.016},
Key = {fds356575}
}
@article{fds310265,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for high-mass diphoton resonances in pp collisions at
s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.92.032004},
Abstract = {This article describes a search for high-mass resonances
decaying to a pair of photons using a sample of 20.3 fb-1 of
pp collisions at s=8 TeV recorded with the ATLAS detector at
the Large Hadron Collider. The data are found to be in
agreement with the Standard Model prediction, and limits are
reported in the framework of the Randall-Sundrum model. This
theory leads to the prediction of graviton states, the
lightest of which could be observed at the Large Hadron
Collider. A lower limit of 2.66 (1.41) TeV at 95% confidence
level is set on the mass of the lightest graviton for
couplings of k/M¯Pl=0.1 (0.01).},
Doi = {10.1103/PhysRevD.92.032004},
Key = {fds310265}
}
@article{fds307963,
Author = {Aaltonen, T and others},
Title = {Search for High-Mass e+e- Resonances in ppbar Collisions at
1.96 TeV},
Journal = {PRL},
Volume = {102},
Number = {3},
Pages = {031801},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.031801},
Abstract = {A search for high-mass resonances in the e+e- final state is
presented based on 2.5 fb(-1) of sqrt[s]=1.96 TeV pp
collision data from the CDF II detector at the Fermilab
Tevatron. The largest excess over the standard model
prediction is at an e+e- invariant mass of 240 GeV/c2. The
probability of observing such an excess arising from
fluctuations in the standard model anywhere in the mass
range of 150-1000 GeV/c2 is 0.6% (equivalent to 2.5sigma).
We exclude the standard model coupling Z' and the
Randall-Sundrum graviton for k/MPl=0.1 with masses below 963
and 848 GeV/c2 at the 95% credibility level,
respectively.},
Doi = {10.1103/physrevlett.102.031801},
Key = {fds307963}
}
@article{fds321081,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for high-mass new phenomena in the dilepton final
state using proton–proton collisions at s=13TeV with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {761},
Pages = {372-392},
Publisher = {Elsevier BV},
Year = {2016},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2016.08.055},
Abstract = {A search is conducted for both resonant and non-resonant
high-mass new phenomena in dielectron and dimuon final
states. The search uses 3.2fb−1 of proton–proton
collision data, collected at s=13TeV by the ATLAS experiment
at the LHC in 2015. The dilepton invariant mass is used as
the discriminating variable. No significant deviation from
the Standard Model prediction is observed; therefore limits
are set on the signal model parameters of interest at 95%
credibility level. Upper limits are set on the cross-section
times branching ratio for resonances decaying to dileptons,
and the limits are converted into lower limits on the
resonance mass, ranging between 2.74 TeV and 3.36 TeV,
depending on the model. Lower limits on the ℓℓqq contact
interaction scale are set between 16.7 TeV and 25.2 TeV,
also depending on the model.},
Doi = {10.1016/j.physletb.2016.08.055},
Key = {fds321081}
}
@article{fds313581,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {Search for high-mass resonances decaying into ZZ in pp̄
collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
ISSN = {1550-7998},
url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000299925100002&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
Abstract = {We search for high-mass resonances decaying into Z boson
pairs using data corresponding to 6fb -1 collected by the
CDF experiment in pp̄ collisions at √s=1.96TeV. The
search is performed in three distinct final states: ZZ→
+-+-, ZZ→ +-νν, and ZZ→ +-jj. For a Randall-Sundrum
graviton G *, the 95% CL upper limits on the production
cross section times branching ratio to ZZ, σ(pp̄→G
*→ZZ), vary between 0.26 pb and 0.045 pb in the mass range
300<M G*<1000GeV/c2. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.85.012008},
Key = {fds313581}
}
@article{fds311114,
Author = {Collaboration, AVKWATLAS},
Title = {Search for high-mass resonances decaying to dilepton final
states in pp collisions at √s = 7 TeV with the ATLAS
detector},
Journal = {JHEP},
Volume = {11},
Number = {11},
Pages = {138},
Publisher = {Springer Nature},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2012)138},
Abstract = {The ATLAS detector at the Large Hadron Collider is used to
search for highmass resonances decaying to an
electron-positron pair or a muon-antimuon pair. The search
is sensitive to heavy neutral Z′ gauge bosons,
Randall-Sundrum gravitons, Z* bosons, techni-mesons,
Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion
models. Results are presented based on an analysis of pp
collisions at a center-of-mass energy of 7 TeV corresponding
to an integrated luminosity of 4.9 fb-1 in the e +e- channel
and 5.0 fb-1 in the μ+μ- channel. A Z′ boson with
Standard Model-like couplings is excluded at 95% confidence
level for masses below 2.22 TeV. A Randall-Sundrum graviton
with coupling k /M̄Pl = 0.1 is excluded at 95% confidence
level for masses below 2.16 TeV. Limits on the other models
are also presented, including Technicolor and Minimal Z′
Models. Copyright CERN.},
Doi = {10.1007/JHEP11(2012)138},
Key = {fds311114}
}
@article{fds311279,
Author = {al, AVKWTAE and Collaboration, CDF},
Title = {Search for High-Mass Resonances Decaying to Dimuons at
CDF},
Journal = {Physical Review Letters},
Volume = {102},
Number = {091805},
Pages = {6},
Year = {2009},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.102.091805},
Abstract = {We present a search for high-mass neutral resonances using
dimuon data corresponding to an integrated luminosity of 2.3
fb(-1) collected in pp[over ] collisions at sqrt[s]=1.96 TeV
by the CDF II detector at the Fermilab Tevatron. No
significant excess above the standard model expectation is
observed in the dimuon invariant-mass spectrum. We set 95%
confidence level upper limits on sigmaBR(pp-->X-->micromicro),
where X is a boson with spin-0, 1, or 2. Using these cross
section limits, we determine lower mass limits on sneutrinos
in R-parity-violating supersymmetric models, Z' bosons, and
Kaluza-Klein gravitons in the Randall-Sundrum
model.},
Doi = {10.1103/physrevlett.102.091805},
Key = {fds311279}
}
@article{fds307960,
Author = {Aaltonen, T and others},
Title = {Search for High-Mass Resonances Decaying to Dimuons at
CDF},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {9},
Pages = {091805},
Publisher = {APS},
Year = {2009},
Month = {Spring},
url = {http://dx.doi.org/10.1103/PhysRevLett.102.091805},
Abstract = {We present a search for high-mass neutral resonances using
dimuon data corresponding to an integrated luminosity of 2.3
fb(-1) collected in pp[over ] collisions at sqrt[s]=1.96 TeV
by the CDF II detector at the Fermilab Tevatron. No
significant excess above the standard model expectation is
observed in the dimuon invariant-mass spectrum. We set 95%
confidence level upper limits on sigmaBR(pp-->X-->micromicro),
where X is a boson with spin-0, 1, or 2. Using these cross
section limits, we determine lower mass limits on sneutrinos
in R-parity-violating supersymmetric models, Z' bosons, and
Kaluza-Klein gravitons in the Randall-Sundrum
model.},
Doi = {10.1103/PhysRevLett.102.091805},
Key = {fds307960}
}
@article{fds308093,
Author = {Abulencia, and A, and others},
Title = {Search for high-mass resonances decaying to e mu in
$p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {21},
Pages = {211802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.211802},
Abstract = {We describe a general search for resonances decaying to a
neutral e mu final state in p anti-p collisions at a
center-of-mass energy of 1.96 TeV. Using a data sample
representing 344 pb-1 of integrated luminosity recorded by
the CDF II experiment, we compare Standard Model predictions
with the number of observed events for invariant masses
between 50 and 800 GeV/c2. Finding no significant excess (5
events observed vs. 7.7 +/- 0.8 expected for M_e mu > 100
GeV/c2), we set limits on sneutrino and Z' masses as
functions of lepton family number violating
couplings.},
Doi = {10.1103/physrevlett.96.211802},
Key = {fds308093}
}
@article{fds347462,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJ and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
Kuutmann, E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz,
AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov,
A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko,
D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer,
F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, J and Chen, S and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard,
AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark, A and Clark, MR},
Title = {Search for High-Mass Resonances Decaying to τν in pp
Collisions at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {120},
Number = {16},
Pages = {161802},
Year = {2018},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.120.161802},
Abstract = {A search for high-mass resonances decaying to τν using
proton-proton collisions at sqrt[s]=13 TeV produced by
the Large Hadron Collider is presented. Only τ-lepton
decays with hadrons in the final state are considered. The
data were recorded with the ATLAS detector and correspond to
an integrated luminosity of 36.1 fb^{-1}. No
statistically significant excess above the standard model
expectation is observed; model-independent upper limits are
set on the visible τν production cross section. Heavy
W^{'} bosons with masses less than 3.7 TeV in the
sequential standard model and masses less than 2.2-3.8 TeV
depending on the coupling in the nonuniversal G(221) model
are excluded at the 95% credibility level.},
Doi = {10.1103/physrevlett.120.161802},
Key = {fds347462}
}
@article{fds310312,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H},
Title = {Search for H→γγ produced in association with top quarks
and constraints on the Yukawa coupling between the top quark
and the Higgs boson using data taken at 7 TeV and 8 TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {740},
Pages = {222-242},
Publisher = {Elsevier BV},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2014.11.049},
Abstract = {A search is performed for Higgs bosons produced in
association with top quarks using the diphoton decay mode of
the Higgs boson. Selection requirements are optimized
separately for leptonic and fully hadronic final states from
the top quark decays. The dataset used corresponds to an
integrated luminosity of 4.5 fb−1 of proton–proton
collisions at a center-of-mass energy of 7 TeV and 20.3
fb−1 at 8 TeV recorded by the ATLAS detector at the CERN
Large Hadron Collider. No significant excess over the
background prediction is observed and upper limits are set
on the tt¯H production cross section. The observed
exclusion upper limit at 95% confidence level is 6.7 times
the predicted Standard Model cross section value. In
addition, limits are set on the strength of the Yukawa
coupling between the top quark and the Higgs boson, taking
into account the dependence of the tt¯H and tH cross
sections as well as the H→γγ branching fraction on the
Yukawa coupling. Lower and upper limits at 95% confidence
level are set at −1.3 and +8.0 times the Yukawa coupling
strength in the Standard Model.},
Doi = {10.1016/j.physletb.2014.11.049},
Key = {fds310312}
}
@article{fds313584,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, E and Arik,
M},
Title = {Search for invisible decays of a Higgs boson produced in
association with a Z boson in ATLAS},
Journal = {Physical Review Letters},
Volume = {112},
Number = {20},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {May},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/PhysRevLett.112.201802},
Abstract = {A search for evidence of invisible-particle decay modes of a
Higgs boson produced in association with a Z boson at the
Large Hadron Collider is presented. No deviation from the
standard model expectation is observed in 4.5 fb-1 (20.3
fb-1) of 7 (8) TeV pp collision data collected by the ATLAS
experiment. Assuming the standard model rate for ZH
production, an upper limit of 75%, at the 95% confidence
level is set on the branching ratio to invisible-particle
decay modes of the Higgs boson at a mass of 125.5 GeV. The
limit on the branching ratio is also interpreted in terms of
an upper limit on the allowed dark matter-nucleon scattering
cross section within a Higgs-portal dark matter scenario.
Within the constraints of such a scenario, the results
presented in this Letter provide the strongest available
limits for low-mass dark matter candidates. Limits are also
set on an additional neutral Higgs boson, in the mass range
110 <mH <400 GeV, produced in association with a Z boson and
decaying to invisible particles.},
Doi = {10.1103/PhysRevLett.112.201802},
Key = {fds313584}
}
@article{fds356784,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for invisible decays of a Higgs boson using
vector-boson fusion in pp collisions at √s=8 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {1},
Pages = {1-44},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2016)172},
Abstract = {A search for a Higgs boson produced via vector-boson fusion
and decaying into invisible particles is presented, using
20.3 fb−1of proton-proton collision data at a
centre-of-mass energy of 8 TeV recorded by the ATLAS
detector at the LHC. For a Higgs boson with a mass of 125
GeV, assuming the Standard Model production cross section,
an upper bound of 0.28 is set on the branching fraction of H
→ invisible at 95% confidence level, where the expected
upper limit is 0.31. The results are interpreted in models
of Higgs-portal dark matter where the branching fraction
limit is converted into upper bounds on the
dark-matter-nucleon scattering cross section as a function
of the dark-matter particle mass, and compared to results
from the direct dark-matter detection experiments.},
Doi = {10.1007/JHEP01(2016)172},
Key = {fds356784}
}
@article{fds310332,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
Title = {Search for invisible decays of the Higgs boson produced in
association with a hadronically decaying vector boson in
pp collisions at [Formula: see text] TeV with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {337},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3551-1},
Abstract = {A search for Higgs boson decays to invisible particles is
performed using 20.3 [Formula: see text] of <i>pp</i>
collision data at a centre-of-mass energy of 8 TeV recorded
by the ATLAS detector at the Large Hadron Collider. The
process considered is Higgs boson production in association
with a vector boson ([Formula: see text] or <i>Z</i>) that
decays hadronically, resulting in events with two or more
jets and large missing transverse momentum. No excess of
candidates is observed in the data over the background
expectation. The results are used to constrain <i>VH</i>
production followed by <i>H</i> decaying to invisible
particles for the Higgs boson mass range [Formula: see
text] GeV. The 95 % confidence-level observed upper limit
on [Formula: see text] varies from 1.6 pb at 115 GeV to
0.13 pb at 300 GeV. Assuming Standard Model production and
including the [Formula: see text] contribution as signal,
the results also lead to an observed upper limit of 78 % at
95 % confidence level on the branching ratio of Higgs
bosons decays to invisible particles at a mass of
125 GeV.},
Doi = {10.1140/epjc/s10052-015-3551-1},
Key = {fds310332}
}
@article{fds356589,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H},
Title = {Search for invisible Higgs boson decays in vector boson
fusion at s=13TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {793},
Pages = {499-519},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1016/j.physletb.2019.04.024},
Abstract = {We report a search for Higgs bosons that are produced via
vector boson fusion and subsequently decay into invisible
particles. The experimental signature is an energetic jet
pair with invariant mass of O(1)TeV and O(100)GeV missing
transverse momentum. The analysis uses 36.1 fb−1 of pp
collision data at s=13TeV recorded by the ATLAS detector at
the LHC. In the signal region the 2252 observed events are
consistent with the background estimation. Assuming a 125GeV
scalar particle with Standard Model cross sections, the
upper limit on the branching fraction of the Higgs boson
decay into invisible particles is 0.37 at 95% confidence
level where 0.28 was expected. This limit is interpreted in
Higgs portal models to set bounds on the WIMP–nucleon
scattering cross section. We also consider invisible decays
of additional scalar bosons with masses up to 3TeV for which
the upper limits on the cross section times branching
fraction are in the range of 0.3–1.7pb.},
Doi = {10.1016/j.physletb.2019.04.024},
Key = {fds356589}
}
@article{fds310318,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Azuelos,
G and Azuma, Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek,
P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil,
HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell,
WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biglietti, M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy,
CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto,
V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron,
J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci,
AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S},
Title = {Search for invisible particles produced in association with
single-top-quarks in proton-proton collisions at [Formula:
see text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {2},
Pages = {79},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-3233-4},
Abstract = {A search for the production of single-top-quarks in
association with missing energy is performed in
proton-proton collisions at a centre-of-mass energy of
[Formula: see text] with the ATLAS experiment at the large
hadron collider using data collected in 2012, corresponding
to an integrated luminosity of [Formula: see
text] fb[Formula: see text]. In this search, the [Formula:
see text] boson from the top quark is required to decay into
an electron or a muon and a neutrino. No deviation from the
standard model prediction is observed, and upper limits are
set on the production cross-section for resonant and
non-resonant production of an invisible exotic state in
association with a right-handed top quark. In the case of
resonant production, for a spin-[Formula: see text]
resonance with a mass of [Formula: see text] GeV, an
effective coupling strength above [Formula: see text] is
excluded at 95[Formula: see text] confidence level for the
top quark and an invisible spin-[Formula: see text] state
with mass between [Formula: see text] and [Formula: see
text] GeV. In the case of non-resonant production, an
effective coupling strength above [Formula: see text] is
excluded at 95[Formula: see text] confidence level for the
top quark and an invisible spin-[Formula: see text] state
with mass between [Formula: see text] and [Formula: see
text] GeV.},
Doi = {10.1140/epjc/s10052-014-3233-4},
Key = {fds310318}
}
@article{fds308183,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett,
JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MA and Cutts, D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Frame, KC and Fuess, S and Gallas, E and Galyaev, AN and Gartung, P and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gibbard, B and Gilmartin, R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grudberg, P and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hahn, KS and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinson, AP and Heintz, U and Heuring, T and Hirosky, R and Hobbs, JD and Hoeneisen, B and Hoftun, JS and Hou, S and Huang, Y and Ito, AS and Jerger, SA and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahn, S and Kajfasz, E and Karmanov, D and Karmgard, D and Kehoe, R and Kim, SK and Klima, B and Klopfenstein, C and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kotwal, AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kuznetsov, VE and Landsberg, G and Leflat, A and Lehner,
F and Li, J and Li, QZ and Lima, JG and Lincoln, D and Linn, SL and Linnemann,
J and Lipton, R and Lucotte, A and Lueking, L and Lundstedt, C and Maciel,
AK and Madaras, RJ and Manankov, V and Mao, HS and Marshall, T and Martin,
MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy,
R and McDonald, J and McMahon, T and Melanson, HL and Meng, XC and Merkin,
M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mincer,
A and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery, HE and Moore,
RW and Mostafa, M and da Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal, HA and Negret, JP and Negroni, S and Norman, D and Oesch, L and Oguri, V and Olivier, B and Oshima, N and Padley, P and Pan,
LJ and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno,
M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Piegaia, R and Piekarz, H and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Quintas, PZ and Raja, R and Rajagopalan,
S and Ramberg, E and Rapidis, PA and Reay, NW and Reucroft, S and Rha, J and Rijssenbeek, M and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sculli, J and Sen, N and Shabalina,
E and Shankar, HC and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell,
RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery,
P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stevenson, ML and Stichelbaut, F and Stoker, D and Stolin, V and Stoyanova, DA and Strauss, M and Streets, K and Strovink,
M and Stutte, L and Sznajder, A and Taylor, W and Tentindo-Repond, S and Thompson, J and Toback, D and Tripathi, SM and Trippe, TG and Turcot,
AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van Kooten and R and Varelas, N and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, Z and Warchol, J and Watts, G and Wayne, M and Weerts, H and White,
A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Wirjawan, JV and Womersley, J and Wood,
DR and Yamada, R and Yamin, P and Yasuda, T and Yip, K and Youssef, S and Yu,
J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zhu, ZH and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev,
EG and Zylberstejn, A},
Title = {Search for large extra dimensions in dielectron and diphoton
production.},
Journal = {Physical review letters},
Volume = {86},
Number = {7},
Pages = {1156-1161},
Year = {2001},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.86.1156},
Abstract = {We report a search for effects of large extra spatial
dimensions in pp collisions at a center-of-mass energy of
1.8 TeV with the D0 detector, using events containing a pair
of electrons or photons. The data are in good agreement with
the expected background and do not exhibit evidence for
large extra dimensions. We set the most restrictive lower
limits to date, at the 95% C.L. on the effective Planck
scale between 1.0 and 1.4 TeV for several formalisms and
numbers of extra dimensions.},
Doi = {10.1103/physrevlett.86.1156},
Key = {fds308183}
}
@article{fds308087,
Author = {Abulencia, and A, and others},
Title = {Search for large extra dimensions in the production of jets
and missing transverse energy in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {17},
Pages = {171802},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.97.171802},
Abstract = {We present the results of a search for new physics in the
jets plus missing transverse energy data sample collected
from 368 pb-1 of p anti-p collisions at s**(1/2) = 1.96 TeV
recorded by the Collider Detector at Fermilab. We compare
the number of events observed in the data with a data-based
estimate of the standard model backgrounds contributing to
this signature. We observe no significant excess of events,
and we interpret this null result in terms of lower limits
on the fundamental Planck scale for a large extra dimensions
scenario.},
Doi = {10.1103/physrevlett.97.171802},
Key = {fds308087}
}
@article{fds356602,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster,
AJ},
Title = {Search for large missing transverse momentum in association
with one top-quark in proton-proton collisions at √s = 13
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2019)041},
Abstract = {This paper describes a search for events with one top-quark
and large missing transverse momentum in the final state.
Data collected during 2015 and 2016 by the ATLAS experiment
from 13 TeV proton–proton collisions at the LHC
corresponding to an integrated luminosity of 36.1 fb −1
are used. Two channels are considered, depending on the
leptonic or the hadronic decays of the W boson from the top
quark. The obtained results are interpreted in the context
of simplified models for dark-matter production and for the
single production of a vector-like T quark. In the absence
of significant deviations from the Standard Model background
expectation, 95% confidence-level upper limits on the
corresponding production cross-sections are obtained and
these limits are translated into constraints on the
parameter space of the models considered.[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP05(2019)041},
Key = {fds356602}
}
@article{fds356648,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Search for lepton-flavor violation in different-flavor,
high-mass final states in pp collisions at s =13 TeV with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {9},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.98.092008},
Abstract = {A search is performed for a heavy particle decaying into
different-flavor, dilepton pairs (eμ, eτ or μτ), using
36.1 fb-1 of proton-proton collision data at s=13 TeV
collected in 2015-2016 by the ATLAS detector at the Large
Hadron Collider. No excesses over the Standard Model
predictions are observed. Bayesian lower limits at the 95%
credibility level are placed on the mass of a Z′ boson,
the mass of a supersymmetric τ-sneutrino, and on the
threshold mass for quantum black-hole production. For the
Z′ and sneutrino models, upper cross-section limits are
converted to upper limits on couplings, which are compared
with similar limits from low-energy experiments and which
are more stringent for the eτ and μτ modes.},
Doi = {10.1103/PhysRevD.98.092008},
Key = {fds356648}
}
@article{fds361985,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin,
RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avner, G and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Badea, A and Bagnaia, P and Bahrasemani, H and Bailey,
AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker,
PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian,
R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Balunas,
WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev,
A and Basan, A and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel,
F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold,
A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde,
B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom,
PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard,
BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Caltabiano, A and Calvente
Lopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero,
J and Cao, Y and Capua, M and Carbone, A and Cardarelli, R and Cardillo, F and Carducci, G and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casadei,
D and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chatterjee, M and Chau, CC and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, CL and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark,
A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement,
C},
Title = {Search for Lepton-Flavor Violation in Z-Boson Decays with τ
Leptons with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {127},
Number = {27},
Pages = {271801},
Year = {2021},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.127.271801},
Abstract = {A search for lepton-flavor-violating Z→eτ and Z→μτ
decays with pp collision data recorded by the ATLAS detector
at the LHC is presented. This analysis uses 139 fb^{-1}
of Run 2 pp collisions at sqrt[s]=13 TeV and is
combined with the results of a similar ATLAS search in the
final state in which the τ lepton decays hadronically,
using the same data set as well as Run 1 data. The addition
of leptonically decaying τ leptons significantly improves
the sensitivity reach for Z→ℓτ decays. The Z→ℓτ
branching fractions are constrained in this analysis to
B(Z→eτ)<7.0×10^{-6} and B(Z→μτ)<7.2×10^{-6} at 95%
confidence level. The combination with the previously
published analyses sets the strongest constraints to date:
B(Z→eτ)<5.0×10^{-6} and B(Z→μτ)<6.5×10^{-6} at 95%
confidence level.},
Doi = {10.1103/physrevlett.127.271801},
Key = {fds361985}
}
@article{fds356649,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Search for lepton-flavor-violating decays of the Z boson
into a τ lepton and a light lepton with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {98},
Number = {9},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.98.092010},
Abstract = {Direct searches for lepton flavor violation in decays of the
Z boson with the ATLAS detector at the LHC are presented.
Decays of the Z boson into an electron or muon and a
hadronically decaying τ lepton are considered. The searches
are based on a data sample of proton-proton collisions
collected by the ATLAS detector in 2015 and 2016,
corresponding to an integrated luminosity of 36.1 fb-1 at a
center-of-mass energy of s=13 TeV. No statistically
significant excess of events above the expected background
is observed, and upper limits on the branching ratios of
lepton-flavor-violating decays are set at the 95% confidence
level: B(Z→eτ)<5.8×10-5 and B(Z→μτ)<2.4×10-5. This
is the first limit on B(Z→eτ) with ATLAS data. The upper
limit on B(Z→μτ) is combined with a previous ATLAS
result based on 20.3 fb-1 of proton-proton collision data at
a center-of-mass energy of s=8 TeV and the combined upper
limit at 95% confidence level is B(Z→μτ)<1.3×10-5.},
Doi = {10.1103/PhysRevD.98.092010},
Key = {fds356649}
}
@article{fds347491,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Noccioli, EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard,
J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán,
SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura,
P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Search for lepton-flavour-violating decays of the Higgs and
Z bosons with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {2},
Pages = {70},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4624-0},
Abstract = {Direct searches for lepton flavour violation in decays of
the Higgs and <i>Z</i> bosons with the ATLAS detector at the
LHC are presented. The following three decays are
considered: [Formula: see text], [Formula: see text], and
[Formula: see text]. The searches are based on the data
sample of proton-proton collisions collected by the ATLAS
detector corresponding to an integrated luminosity of
20.3 [Formula: see text] at a centre-of-mass energy of
[Formula: see text] TeV. No significant excess is observed,
and upper limits on the lepton-flavour-violating branching
ratios are set at the 95[Formula: see text] confidence
level: Br[Formula: see text], Br[Formula: see text], and
Br[Formula: see text].},
Doi = {10.1140/epjc/s10052-017-4624-0},
Key = {fds347491}
}
@article{fds348987,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for lepton-flavour-violating H → μτ decays of the
Higgs boson with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {11},
Pages = {1-33},
Year = {2015},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2015)211},
Abstract = {A direct search for lepton-flavour-violating H → μτ
decays of the recently discovered Higgs boson with the ATLAS
detector at the LHC is presented. The analysis is performed
in the H → μτhad channel, where τhad is a hadronically
decaying τ -lepton. The search is based on the data sample
of proton-proton collisions collected by the ATLAS
experiment corresponding to an integrated luminosity of 20.3
fb−1 at a centre-of-mass energy of TeV. No statistically
significant excess of data over the predicted background is
observed. The observed (expected) 95% confidence-level upper
limit on the branching fraction, Br(H → μτ ), is 1.85%
(1.24%).[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP11(2015)211},
Key = {fds348987}
}
@article{fds308173,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko,
LV},
Title = {Search for Leptoquark Pairs Decaying into [Formula
presented] in [Formula presented] Collisions at [Formula
presented]},
Journal = {Physical Review Letters},
Volume = {88},
Number = {19},
Pages = {7},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.88.191801},
Abstract = {We present the results of a search for leptoquark (LQ) pairs
in [Formula presented] of [Formula presented] collider data
collected by the D0 experiment at the Fermilab Tevatron. We
observe no evidence for leptoquark production and set a
limit on [Formula presented] as a function of the mass of
the leptoquark [Formula presented]. Assuming the decay
[Formula presented], we exclude scalar leptoquarks for
[Formula presented], and vector leptoquarks for [Formula
presented] and coupling which produces the minimum cross
section, at a [Formula presented] confidence level. © 2002
The American Physical Society.},
Doi = {10.1103/PhysRevLett.88.191801},
Key = {fds308173}
}
@article{fds350338,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz, VA and Pereira,
RA},
Title = {Search for light long-lived neutral particles produced in pp
collisions at √s=13TeV and decaying into collimated
leptons or light hadrons with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {5},
Year = {2020},
Month = {May},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-7997-4},
Abstract = {Several models of physics beyond the Standard Model predict
the existence of dark photons, light neutral particles
decaying into collimated leptons or light hadrons. This
paper presents a search for long-lived dark photons produced
from the decay of a Higgs boson or a heavy scalar boson and
decaying into displaced collimated Standard Model fermions.
The search uses data corresponding to an integrated
luminosity of 36.1 fb- 1 collected in proton–proton
collisions at s=13 Te recorded in 2015–2016 with the
ATLAS detector at the Large Hadron Collider. The observed
number of events is consistent with the expected background,
and limits on the production cross section times branching
fraction as a function of the proper decay length of the
dark photon are reported. A cross section times branching
fraction above 4 pb is excluded for a Higgs boson decaying
into two dark photons for dark-photon decay lengths between
1.5 mm and 307 mm.},
Doi = {10.1140/epjc/s10052-020-7997-4},
Key = {fds350338}
}
@article{fds356629,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O},
Title = {Search for light resonances decaying to boosted quark pairs
and produced in association with a photon or a jet in
proton–proton collisions at √s=13TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {788},
Pages = {316-335},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2018.09.062},
Abstract = {This Letter presents a search for new light resonances
decaying to pairs of quarks and produced in association with
a high-pT photon or jet. The dataset consists of
proton–proton collisions with an integrated luminosity of
36.1 fb−1 at a centre-of-mass energy of s=13 TeV recorded
by the ATLAS detector at the Large Hadron Collider.
Resonance candidates are identified as massive large-radius
jets with substructure consistent with a particle decaying
into a quark pair. The mass spectrum of the candidates is
examined for local excesses above background. No evidence of
a new resonance is observed in the data, which are used to
exclude the production of a lepto-phobic axial-vector Z′
boson.},
Doi = {10.1016/j.physletb.2018.09.062},
Key = {fds356629}
}
@article{fds307673,
Author = {ATLAS Collaboration},
Title = {Search for light top squark pair production in final states
with leptons and b-jets with the ATLAS detector in sqrt(s) =
7 TeV proton-proton collisions},
Journal = {Physics Letters B},
Volume = {72},
Number = {11},
Publisher = {Springer Nature},
Year = {2012},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2237-1},
Abstract = {A search is presented for the pair production of light
scalar top quarks in √s = 7 TeV proton–proton collisions
recorded with the ATLAS detector at the Large Hadron
Collider. This analysis uses the full data sample collected
during 2011 running that corresponds to a total integrated
luminosity of 4.7 fb−1. Light scalar top quarks are
searched for in events with two opposite-sign leptons (e,
μ), large missing transverse momentum and at least one jet
in the final state. No excess over Standard Model
expectations is found, and the results are interpreted under
the assumption that the light scalar top decays to a b-quark
in addition to an on-shell chargino whose decay occurs
through a virtual W boson. If the chargino mass is 106 GeV,
light scalar top-quark masses up to 130 GeV are excluded for
neutralino masses below 70 GeV.},
Doi = {10.1140/epjc/s10052-012-2237-1},
Key = {fds307673}
}
@article{fds307610,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Search for light top squark pair production in final states
with leptons and b-jets with the ATLAS detector in √s=7
TeV proton–proton collisions},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {720},
Number = {1-3},
Pages = {13-31},
Publisher = {Elsevier BV},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.049},
Abstract = {The results of a search for pair production of light top
squarks are presented, using 4.7 fb−1 of s=7 TeV
proton–proton collisions collected with the ATLAS detector
at the Large Hadron Collider. This search targets top
squarks with masses similar to, or lighter than, the top
quark mass. Final states containing exclusively one or two
leptons (e,μ), large missing transverse momentum,
light-flavour jets and b-jets are used to reconstruct the
top squark pair system. Event-based mass scale variables are
used to separate the signal from a large tt¯ background. No
excess over the Standard Model expectations is found. The
results are interpreted in the framework of the Minimal
Supersymmetric Standard Model, assuming the top squark
decays exclusively to a chargino and a b-quark, while
requiring different mass relationships between the
Supersymmetric particles in the decay chain. Light top
squarks with masses between 123–167 GeV are excluded for
neutralino masses around 55 GeV.},
Doi = {10.1016/j.physletb.2013.01.049},
Key = {fds307610}
}
@article{fds356681,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Search for long-lived charginos based on a
disappearing-track signature in pp collisions at √s=13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {6},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2018)022},
Abstract = {This paper presents a search for direct electroweak gaugino
or gluino pair production with a chargino nearly
mass-degenerate with a stable neutralino. It is based on an
integrated luminosity of 36.1 fb−1 of pp collisions at
s=13 TeV collected by the ATLAS experiment at the LHC. The
final state of interest is a disappearing track accompanied
by at least one jet with high transverse momentum from
initial-state radiation or by four jets from the gluino
decay chain. The use of short track segments reconstructed
from the innermost tracking layers significantly improves
the sensitivity to short chargino lifetimes. The results are
found to be consistent with Standard Model predictions.
Exclusion limits are set at 95% confidence level on the mass
of charginos and gluinos for different chargino lifetimes.
For a pure wino with a lifetime of about 0.2 ns, chargino
masses up to 460 GeV are excluded. For the strong production
channel, gluino masses up to 1.65 TeV are excluded assuming
a chargino mass of 460 GeV and lifetime of 0.2 ns.[Figure
not available: see fulltext.].},
Doi = {10.1007/JHEP06(2018)022},
Key = {fds356681}
}
@article{fds364957,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling, JH},
Title = {Search for long-lived charginos based on a
disappearing-track signature using 136 fb - 1 of
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {7},
Year = {2022},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10489-5},
Abstract = {A search for long-lived charginos produced either directly
or in the cascade decay of heavy prompt gluino states is
presented. The search is based on proton–proton collision
data collected at a centre-of-mass energy of s = 13 TeV
between 2015 and 2018 with the ATLAS detector at the LHC,
corresponding to an integrated luminosity of 136 fb- 1.
Long-lived charginos are characterised by a distinct
signature of a short and then disappearing track, and are
reconstructed using at least four measurements in the ATLAS
pixel detector, with no subsequent measurements in the
silicon-microstrip tracking volume nor any associated energy
deposits in the calorimeter. The final state is complemented
by a large missing transverse-momentum requirement for
triggering purposes and at least one high-transverse-momentum
jet. No excess above the expected backgrounds is observed.
Exclusion limits are set at 95% confidence level on the
masses of the chargino and gluino for different chargino
lifetimes. Chargino masses up to 660 (210) GeV are
excluded in scenarios where the chargino is a pure wino
(higgsino). For charginos produced during the cascade decay
of a heavy gluino, gluinos with masses below 2.1 TeV are
excluded for a chargino mass of 300 GeV and a lifetime of
0.2 ns.},
Doi = {10.1140/epjc/s10052-022-10489-5},
Key = {fds364957}
}
@article{fds308130,
Author = {al, AVKWDAE},
Title = {Search for Long-Lived Doubly-Charged Higgs Bosons in P
anti-P Collisions at s**(1/2) = 1.96 TeV},
Journal = {Physical Review Letters},
Volume = {95},
Number = {071801},
Year = {2005},
Month = {August},
Key = {fds308130}
}
@article{fds307949,
Author = {Aaltonen, T and others},
Title = {Search for Long-Lived Massive Charged Particles in 1.96 TeV
pp̅ Collisions},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {2},
Pages = {021802},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.021802},
Abstract = {We performed a signature-based search for long-lived charged
massive particles produced in 1.0 fb-1 of pp̅
collisions at sqrt[s]=1.96 TeV, collected with the CDF
II detector using a high transverse-momentum (pT) muon
trigger. The search used time of flight to isolate slowly
moving, high-pT particles. One event passed our selection
cuts with an expected background of 1.9 ± 0.2 events.
We set an upper bound on the production cross section and,
interpreting this result within the context of a stable
scalar top-quark model, set a lower limit on the particle
mass of 249 GeV/c2 at 95% C.L.},
Doi = {10.1103/physrevlett.103.021802},
Key = {fds307949}
}
@article{fds310347,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for long-lived neutral particles decaying into lepton
jets in proton-proton collisions at √s= 8TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {11},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP11(2014)088},
Abstract = {Abstract: Several models of physics beyond the Standard
Model predict neutral particles that decay into final states
consisting of collimated jets of light leptons and hadrons
(so-called “lepton jets”). These particles can also be
long-lived with decay length comparable to, or even larger
than, the LHC detectors’ linear dimensions. This paper
presents the results of a search for lepton jets in
proton-proton collisions at the centre-of-mass energy of
√s= 8TeV in a sample of 20.3 fb−1 collected during 2012
with the ATLAS detector at the LHC. Limits on models
predicting Higgs boson decays to neutral long-lived lepton
jets are derived as a function of the particle’s proper
decay length.},
Doi = {10.1007/JHEP11(2014)088},
Key = {fds310347}
}
@article{fds356592,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger,
M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou,
C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Estevez, MA and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Bella, LA and Arabidze, G and Araque, JP and Ferraz,
VA and Pereira, RA and Arce, ATH and Arduh, FA and Arguin,
JF},
Title = {Search for long-lived neutral particles in pp collisions at
√s=13TeV that decay into displaced hadronic jets in the
ATLAS calorimeter},
Journal = {European Physical Journal C},
Volume = {79},
Number = {6},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-6962-6},
Abstract = {This paper describes a search for pairs of neutral,
long-lived particles decaying in the ATLAS calorimeter.
Long-lived particles occur in many extensions to the
Standard Model and may elude searches for new promptly
decaying particles. The analysis considers neutral,
long-lived scalars with masses between 5 and 400 GeV,
produced from decays of heavy bosons with masses between 125
and 1000 GeV, where the long-lived scalars decay into
Standard Model fermions. The analysis uses either 10.8fb-1
or 33.0fb-1 of data (depending on the trigger) recorded in
2016 at the LHC with the ATLAS detector in proton–proton
collisions at a centre-of-mass energy of 13 TeV. No
significant excess is observed, and limits are reported on
the production cross section times branching ratio as a
function of the proper decay length of the long-lived
particles.},
Doi = {10.1140/epjc/s10052-019-6962-6},
Key = {fds356592}
}
@article{fds349432,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
Title = {Search for long-lived neutral particles produced in pp
collisions at s =13 TeV decaying into displaced hadronic
jets in the ATLAS inner detector and muon
spectrometer},
Journal = {Physical Review D},
Volume = {101},
Number = {5},
Year = {2020},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.101.052013},
Abstract = {A search is presented for pair production of long-lived
neutral particles using 33 fb-1 of s=13 TeV proton-proton
collision data, collected during 2016 by the ATLAS detector
at the LHC. This search focuses on a topology in which one
long-lived particle decays in the ATLAS inner detector and
the other decays in the muon spectrometer. Special
techniques are employed to reconstruct the displaced tracks
and vertices in the inner detector and in the muon
spectrometer. One event is observed that passes the full
event selection, which is consistent with the estimated
background. Limits are placed on scalar boson propagators
with masses from 125 GeV to 1000 GeV decaying into pairs of
long-lived hidden-sector scalars with masses from 8 GeV to
400 GeV. The limits placed on several low-mass scalars
extend previous exclusion limits in the range of proper
lifetimes cτ from 5 cm to 1 m.},
Doi = {10.1103/PhysRevD.101.052013},
Key = {fds349432}
}
@article{fds347448,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Search for long-lived particles in final states with
displaced dimuon vertices in pp collisions at s =13 TeV with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {99},
Number = {1},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.99.012001},
Abstract = {A search is performed for a long-lived particle decaying
into a final state that includes a pair of muons of
opposite-sign electric charge, using proton-proton collision
data collected at s=13 TeV by the ATLAS detector at the
Large Hadron Collider corresponding to an integrated
luminosity of 32.9 fb-1. No significant excess over the
Standard Model expectation is observed. Limits at 95%
confidence level on the lifetime of the long-lived particle
are presented in models of new phenomena including
gauge-mediated supersymmetry or decay of the Higgs boson, H,
to a pair of dark photons, ZD. Lifetimes in the range
cτ=1-2400 cm are excluded, depending on the parameters of
the model. In the supersymmetric model, the lightest
neutralino is the next-to-lightest supersymmetric particle,
with a relatively long lifetime due to its weak coupling to
the gravitino, the lightest supersymmetric particle. The
lifetime limits are determined for very light gravitino mass
and various assumptions for the neutralino mass in the range
300-1000 GeV. In the dark photon model, the lifetime limits
are interpreted as exclusion contours in the plane of the
coupling between the ZD and the Standard Model Z boson
versus the ZD mass (in the range 20-60 GeV), for various
assumptions for the H→ZDZD branching fraction.},
Doi = {10.1103/PhysRevD.99.012001},
Key = {fds347448}
}
@article{fds356620,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for long-lived particles produced in pp collisions at
s =13 TeV that decay into displaced hadronic jets in the
ATLAS muon spectrometer},
Journal = {Physical Review D},
Volume = {99},
Number = {5},
Year = {2019},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.99.052005},
Abstract = {A search for the decay of neutral, weakly interacting,
long-lived particles using data collected by the ATLAS
detector at the LHC is presented. The analysis in this paper
uses 36.1 fb-1 of proton-proton collision data at s=13 TeV
recorded in 2015-2016. The search employs techniques for
reconstructing vertices of long-lived particles decaying
into jets in the muon spectrometer exploiting a two-vertex
strategy and a novel technique that requires only one vertex
in association with additional activity in the detector that
improves the sensitivity for longer lifetimes. The observed
numbers of events are consistent with the expected
background and limits for several benchmark signals are
determined.},
Doi = {10.1103/PhysRevD.99.052005},
Key = {fds356620}
}
@article{fds311113,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abou Zeid and OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for long-lived stopped R-hadrons decaying out of time
with pp collisions using the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {11},
Pages = {112003-1-112003-30},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.88.112003},
Abstract = {An updated search is performed for gluino, top squark, or
bottom squark R-hadrons that have come to rest within the
ATLAS calorimeter, and decay at some later time to hadronic
jets and a neutralino, using 5.0 and 22:9 fb-1 of pp
collisions at 7 and 8 TeV, respectively. Candidate decay
events are triggered in selected empty bunch crossings of
the LHC in order to remove pp collision backgrounds.
Selections based on jet shape and muon system activity are
applied to discriminate signal events from cosmic ray and
beam-halo muon backgrounds. In the absence of an excess of
events, improved limits are set on gluino, stop, and sbottom
masses for different decays, lifetimes, and neutralino
masses. With a neutralino of mass 100 GeV, the analysis
excludes gluinos with mass below 832 GeV (with an expected
lower limit of 731 GeV), for a gluino lifetime between 10
μs and 1000 s in the generic R-hadron model with equal
branching ratios for decays to (formula presented) and
(formula presented). Under the same assumptions for the
neutralino mass and squark lifetime, top squarks and bottom
squarks in the Regge R-hadron model are excluded with masses
below 379 and 344 GeV, respectively.},
Doi = {10.1103/PhysRevD.88.112003},
Key = {fds311113}
}
@article{fds307622,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio
Bella, L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce,
ATH and Arfaoui, S and Arguin, JF and Arik, E},
Title = {Search for long-lived, heavy particles in final states with
a muon and multi-track displaced vertex in proton-proton
collisions at √s=7 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {719},
Number = {4-5},
Pages = {280-298},
Publisher = {Elsevier BV},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.042},
Abstract = {Many extensions of the Standard Model posit the existence of
heavy particles with long lifetimes. In this Letter, results
are presented of a search for events containing one or more
such particles, which decay at a significant distance from
their production point, using a final state containing
charged hadrons and an associated muon. This analysis uses a
data sample of proton-proton collisions at s=7TeV
corresponding to an integrated luminosity of 4.4 fb−1
collected in 2011 by the ATLAS detector operating at the
Large Hadron Collider. Results are interpreted in the
context of R-parity violating supersymmetric scenarios. No
events in the signal region are observed and limits are set
on the production cross section for pair production of
supersymmetric particles, multiplied by the square of the
branching fraction for a neutralino to decay to charged
hadrons and a muon, based on the scenario where both of the
produced supersymmetric particles give rise to neutralinos
that decay in this way. However, since the search strategy
is based on triggering on and reconstructing the decay
products of individual long-lived particles, irrespective of
the rest of the event, these limits can easily be
reinterpreted in scenarios with different numbers of
long-lived particles per event. The limits are presented as
a function of neutralino lifetime, and for a range of squark
and neutralino masses.},
Doi = {10.1016/j.physletb.2013.01.042},
Key = {fds307622}
}
@article{fds353484,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Search for long-lived, massive particles in events with a
displaced vertex and a muon with large impact parameter in
pp collisions at s =13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {102},
Number = {3},
Year = {2020},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.102.032006},
Abstract = {A search for long-lived particles decaying into hadrons and
at least one muon is presented. The analysis selects events
that pass a muon or missing-transverse-momentum trigger and
contain a displaced muon track and a displaced vertex. The
analyzed dataset of proton-proton collisions at s=13 TeV was
collected with the ATLAS detector and corresponds to 136
fb-1. The search employs dedicated reconstruction techniques
that significantly increase the sensitivity to long-lived
particle decays that occur in the ATLAS inner detector.
Background estimates for Standard Model processes and
instrumental effects are extracted from data. The observed
event yields are compatible with those expected from
background processes. The results are presented as limits at
95% confidence level on model-independent cross sections for
processes beyond the Standard Model, and interpreted as
exclusion limits in scenarios with pair production of
long-lived top squarks that decay via a small
R-parity-violating coupling into a quark and a muon. Top
squarks with masses up to 1.7 TeV are excluded for a
lifetime of 0.1 ns, and masses below 1.3 TeV are excluded
for lifetimes between 0.01 ns and 30 ns.},
Doi = {10.1103/PhysRevD.102.032006},
Key = {fds353484}
}
@article{fds356694,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Search for long-lived, massive particles in events with
displaced vertices and missing transverse momentum in √s =
13 TeV pp collisions with the ATLAS detector},
Journal = {Physical Review D},
Volume = {97},
Number = {5},
Year = {2018},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.97.052012},
Abstract = {A search for long-lived, massive particles predicted by many
theories beyond the Standard Model is presented. The search
targets final states with large missing transverse momentum
and at least one high-mass displaced vertex with five or
more tracks, and uses 32.8 fb-1 of s=13 TeV pp collision
data collected by the ATLAS detector at the LHC. The
observed yield is consistent with the expected background.
The results are used to extract 95% C.L. exclusion limits on
the production of long-lived gluinos with masses up to 2.37
TeV and lifetimes of O(10-2)-O(10) ns in a simplified model
inspired by split supersymmetry.},
Doi = {10.1103/PhysRevD.97.052012},
Key = {fds356694}
}
@article{fds356788,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux,
ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos,
S and Arik, E and Arik, M},
Title = {Search for long-lived, multi-charged particles in pp
collisions at √s=7 TeV using the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {722},
Number = {4-5},
Pages = {305-323},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2013.04.036},
Abstract = {A search for highly ionising, penetrating particles with
electric charges from |q|=2e to 6e is performed using the
ATLAS detector at the CERN Large Hadron Collider.
Proton-proton collision data taken at s=7 TeV during the
2011 running period, corresponding to an integrated
luminosity of 4.4 fb−1, are analysed. No signal candidates
are observed, and 95% confidence level cross-section upper
limits are interpreted as mass-exclusion lower limits for a
simplified Drell–Yan production model. In this model,
masses are excluded from 50 GeV up to 430, 480, 490, 470 and
420 GeV for charges 2e, 3e, 4e, 5e and 6e,
respectively.},
Doi = {10.1016/j.physletb.2013.04.036},
Key = {fds356788}
}
@article{fds310275,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for long-lived, weakly interacting particles that
decay to displaced hadronic jets in proton-proton collisions
at s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.92.012010},
Abstract = {A search for the decay of neutral, weakly interacting,
long-lived particles using data collected by the ATLAS
detector at the LHC is presented. This analysis uses the
full data set recorded in 2012: 20.3 fb-1 of proton-proton
collision data at s=8 TeV. The search employs techniques for
reconstructing decay vertices of long-lived particles
decaying to jets in the inner tracking detector and muon
spectrometer. Signal events require at least two
reconstructed vertices. No significant excess of events over
the expected background is found, and limits as a function
of proper lifetime are reported for the decay of the Higgs
boson and other scalar bosons to long-lived particles and
for Hidden Valley Z′ and Stealth SUSY benchmark models.
The first search results for displaced decays in Z′ and
Stealth SUSY models are presented. The upper bounds of the
excluded proper lifetimes are the most stringent to
date.},
Doi = {10.1103/PhysRevD.92.012010},
Key = {fds310275}
}
@article{fds347458,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund,
O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RMB and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M},
Title = {Search for Low-Mass Dijet Resonances Using Trigger-Level
Jets with the ATLAS Detector in pp Collisions at
sqrt[s]=13 TeV.},
Journal = {Physical review letters},
Volume = {121},
Number = {8},
Pages = {081801},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.121.081801},
Abstract = {Searches for dijet resonances with sub-TeV masses using the
ATLAS detector at the Large Hadron Collider can be
statistically limited by the bandwidth available to
inclusive single-jet triggers, whose data-collection rates
at low transverse momentum are much lower than the rate from
standard model multijet production. This Letter describes a
new search for dijet resonances where this limitation is
overcome by recording only the event information calculated
by the jet trigger algorithms, thereby allowing much higher
event rates with reduced storage needs. The search targets
low-mass dijet resonances in the range 450-1800 GeV. The
analyzed data set has an integrated luminosity of up to
29.3 fb^{-1} and was recorded at a center-of-mass
energy of 13 TeV. No excesses are found; limits are set on
Gaussian-shaped contributions to the dijet mass distribution
from new particles and on a model of dark-matter particles
with axial-vector couplings to quarks.},
Doi = {10.1103/physrevlett.121.081801},
Key = {fds347458}
}
@article{fds347551,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed
Abud, A and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham,
NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras,
D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V},
Title = {Search for low-mass resonances decaying into two jets and
produced in association with a photon using pp collisions at
s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {795},
Pages = {56-75},
Year = {2019},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2019.03.067},
Abstract = {A search is performed for localised excesses in dijet mass
distributions of low-dijet-mass events produced in
association with a high transverse energy photon. The search
uses up to 79.8 fb−1 of LHC proton–proton collisions
collected by the ATLAS experiment at a centre-of-mass energy
of 13 TeV during 2015–2017. Two variants are presented:
one which makes no jet flavour requirements and one which
requires both jets to be tagged as b-jets. The observed mass
distributions are consistent with multi-jet processes in the
Standard Model. The data are used to set upper limits on the
production cross-section for a benchmark Z′ model and,
separately, on generic Gaussian-shape contributions to the
mass distributions, extending the current ATLAS constraints
on dijet resonances to the mass range between 225 and 1100
GeV.},
Doi = {10.1016/j.physletb.2019.03.067},
Key = {fds347551}
}
@article{fds310276,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for low-scale gravity signatures in multi-jet final
states with the ATLAS detector at √s =
8TeV},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {7},
Publisher = {Springer Nature},
Year = {2015},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2015)032},
Abstract = {A search for evidence of physics beyond the Standard Model
in final states with multiple high-transverse-momentum jets
is performed using 20.3 fb−1 of proton-proton collision
data at (Formula presented.) = 8 TeV recorded by the ATLAS
detector at the LHC. No significant excess of events beyond
Standard Model expectations is observed, and upper limits on
the visible cross sections for non-Standard Model production
of multi-jet final states are set. A wide variety of models
for black hole and string ball production and decay are
considered, and the upper limit on the cross section times
acceptance is as low as 0.16 fb at the 95% confidence level.
For these models, excluded regions are also given as
function of the main model parameters.},
Doi = {10.1007/JHEP07(2015)032},
Key = {fds310276}
}
@article{fds348981,
Author = {Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Achkar, B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R and Arcangeletti, C and Arce, ATH and Arduh, FA and Arguin,
J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O and Arnold, H and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Augsten, K and Avolio, G and Avramidou,
R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baca, MJ and Bachacou,
H and Bachas, K and Backes, M and Backman, F and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura,
AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barsov, S and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Berry, T and Berta, P and Bertella, C and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi,
M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bitadze, A and Bittrich, C and Bjørke, K and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock,
I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bührer, F and Bulekov, O and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burr, JTP and Burzynski, JC and Büscher, V and Buschmann, E and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Capua, M and Cardarelli, R and Cardillo, FC and Carducci, G and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carter, JWS and Casado, MP and Casha, AF and Casper,
DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chakraborty, D and Chan, SK and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chau, CC and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen,
Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias,
TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ},
Title = {Search for Magnetic Monopoles and Stable
High-Electric-Charge Objects in 13 Tev Proton-Proton
Collisions with the ATLAS Detector.},
Journal = {Physical review letters},
Volume = {124},
Number = {3},
Pages = {031802},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.124.031802},
Abstract = {A search for magnetic monopoles and high-electric-charge
objects is presented using 34.4 fb^{-1} of 13 TeV pp
collision data collected by the ATLAS detector at the LHC
during 2015 and 2016. The considered signature is based upon
high ionization in the transition radiation tracker of the
inner detector associated with a pencil-shape energy deposit
in the electromagnetic calorimeter. The data were collected
by a dedicated trigger based on the tracker high-threshold
hit capability. The results are interpreted in models of
Drell-Yan pair production of stable particles with two spin
hypotheses (0 and 1/2) and masses ranging from 200 to
4000 GeV. The search improves by approximately a factor of
5 the constraints on the direct production of magnetic
monopoles carrying one or two Dirac magnetic charges and
stable objects with electric charge in the range
20≤|z|≤60 and extends the charge range to
60<|z|≤100.},
Doi = {10.1103/physrevlett.124.031802},
Key = {fds348981}
}
@article{fds315362,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for magnetic monopoles and stable particles with high
electric charges in 8 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {93},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {March},
ISSN = {2470-0010},
url = {http://dx.doi.org/10.1103/PhysRevD.93.052009},
Abstract = {A search for highly ionizing particles produced in
proton-proton collisions at 8 TeV center-of-mass energy is
performed by the ATLAS Collaboration at the CERN Large
Hadron Collider. The data set used corresponds to an
integrated luminosity of 7.0 fb-1. A customized trigger
significantly increases the sensitivity, permitting a search
for such particles with charges and energies beyond what was
previously accessible. No events were found in the signal
region, leading to production cross section upper limits in
the mass range 200-2500 GeV for magnetic monopoles with
magnetic charge in the range 0.5gD<|g|<2.0gD, where gD is
the Dirac charge, and for stable particles with electric
charge in the range 10<|z|<60. Model-dependent limits are
presented in given pair-production scenarios, and
model-independent limits are presented in fiducial regions
of particle energy and pseudorapidity.},
Doi = {10.1103/PhysRevD.93.052009},
Key = {fds315362}
}
@article{fds307654,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert,
B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou,
R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow,
T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch,
V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker,
AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Begel, M and Behar Harpaz and S and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo
Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J},
Title = {Search for magnetic monopoles in sqrt[s]=7 TeV pp
collisions with the ATLAS detector.},
Journal = {Physical review letters},
Volume = {109},
Number = {26},
Pages = {261803},
Year = {2012},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.109.261803},
Abstract = {This Letter presents a search for magnetic monopoles with
the ATLAS detector at the CERN Large Hadron Collider using
an integrated luminosity of 2.0 fb(-1) of pp collisions
recorded at a center-of-mass energy of sqrt[s]=7 TeV.
No event is found in the signal region, leading to an upper
limit on the production cross section at 95% confidence
level of 1.6/ϵ fb for Dirac magnetic monopoles with
the minimum unit magnetic charge and with mass between 200
GeV and 1500 GeV, where ϵ is the monopole reconstruction
efficiency. The efficiency ϵ is high and uniform in the
fiducial region given by pseudorapidity |η|<1.37 and
transverse kinetic energy 600-700<E(kin)sinθ<1400 GeV.
The minimum value of 700 GeV is for monopoles of mass 200
GeV, whereas the minimum value of 600 GeV is applicable for
higher mass monopoles. Therefore, the upper limit on the
production cross section at 95% confidence level is 2 fb in
this fiducial region. Assuming the kinematic distributions
from Drell-Yan pair production of spin-1/2 Dirac magnetic
monopoles, the efficiency is in the range 1%-10%, leading to
an upper limit on the cross section at 95% confidence level
that varies from 145 fb to 16 fb for monopoles with mass
between 200 GeV and 1200 GeV. This limit is weaker than the
fiducial limit because most of these monopoles lie outside
the fiducial region.},
Doi = {10.1103/physrevlett.109.261803},
Key = {fds307654}
}
@article{fds372888,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Khoury,
KA and Alberghi, GL and Albert, J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Search for Majorana neutrinos in same-sign WW scattering
events from pp collisions at √s=13 TeV},
Journal = {European Physical Journal C},
Volume = {83},
Number = {9},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11915-y},
Abstract = {A search for Majorana neutrinos in same-sign WW scattering
events is presented. The analysis uses s=13 TeV
proton–proton collision data with an integrated luminosity
of 140 fb - 1 recorded during 2015–2018 by the ATLAS
detector at the Large Hadron Collider. The analysis targets
final states including exactly two same-sign muons and at
least two hadronic jets well separated in rapidity. The
modelling of the main backgrounds, from Standard Model
same-sign WW scattering and WZ production, is constrained
with data in dedicated signal-depleted control regions. The
distribution of the transverse momentum of the
second-hardest muon is used to search for signals
originating from a heavy Majorana neutrino with a mass
between 50 GeV and 20 TeV. No significant excess is
observed over the background expectation. The results are
interpreted in a benchmark scenario of the Phenomenological
Type-I Seesaw model. In addition, the sensitivity to the
Weinberg operator is investigated. Upper limits at the 95%
confidence level are placed on the squared
muon-neutrino–heavy-neutrino mass-mixing matrix element |
VμN| 2 as a function of the heavy Majorana neutrino’s
mass mN , and on the effective μμ Majorana neutrino mass |
mμμ| .},
Doi = {10.1140/epjc/s10052-023-11915-y},
Key = {fds372888}
}
@article{fds325310,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TP and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amoros, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimaraes da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Boeser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler,
S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans,
G and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Buescher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
JM and Buttinger, W and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale,
V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido,
MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan,
M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall,
J},
Title = {Search for massive colored scalars in four-jet final states
in √s=7 TeV proton-proton collisions with the ATLAS
detector},
Journal = {EUROPEAN PHYSICAL JOURNAL C},
Volume = {71},
Number = {12},
Publisher = {Springer New York LLC},
Year = {2011},
url = {http://dx.doi.org/10.1140/epjc/s10052-011-1828-6},
Abstract = {A search for pair-produced scalar particles decaying to a
four-jet final state is presented. The analysis is performed
using an integrated luminosity of 34 pb-1 recorded by the
ATLAS detector in 2010. No deviation from the Standard Model
is observed. For a scalar mass of 100 GeV (190 GeV) the
limit on the scalar gluon pair production cross section at
95% confidence level is 1 nb (0.28 nb). When these results
are interpreted as mass limits, scalar-gluons (hyperpions)
with masses of 100 to 185 GeV (100 to 155 GeV) are excluded
at 95% confidence level with the exception of a mass window
of width about 5 GeV (15 GeV) around 140
GeV.},
Doi = {10.1140/epjc/s10052-011-1828-6},
Key = {fds325310}
}
@article{fds310280,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for massive supersymmetric particles decaying to many
jets using the ATLAS detector in pp collisions at s =8
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.91.112016},
Abstract = {Results of a search for decays of massive particles to fully
hadronic final states are presented. This search uses 20.3
fb-1 of data collected by the ATLAS detector in s=8 TeV
proton-proton collisions at the LHC. Signatures based on
high jet multiplicities without requirements on the missing
transverse momentum are used to search for
R-parity-violating supersymmetric gluino pair production
with subsequent decays to quarks. The analysis is performed
using a requirement on the number of jets, in combination
with separate requirements on the number of b-tagged jets,
as well as a topological observable formed from the scalar
sum of the mass values of large-radius jets in the event.
Results are interpreted in the context of all possible
branching ratios of direct gluino decays to various quark
flavors. No significant deviation is observed from the
expected Standard Model backgrounds estimated using jet
counting as well as data-driven templates of the
total-jet-mass spectra. Gluino pair decays to ten or more
quarks via intermediate neutralinos are excluded for a
gluino with mass mg<1 TeV for a neutralino mass mχ10=500
GeV. Direct gluino decays to six quarks are excluded for
mg<917 GeV for light-flavor final states, and results for
various flavor hypotheses are presented.},
Doi = {10.1103/PhysRevD.91.112016},
Key = {fds310280}
}
@article{fds313606,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for massive, long-lived particles using multitrack
displaced vertices or displaced lepton pairs in pp
collisions at s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {October},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.92.072004},
Abstract = {Many extensions of the Standard Model posit the existence of
heavy particles with long lifetimes. This article presents
the results of a search for events containing at least one
long-lived particle that decays at a significant distance
from its production point into two leptons or into five or
more charged particles. This analysis uses a data sample of
proton-proton collisions at s=8 TeV corresponding to an
integrated luminosity of 20.3 fb-1 collected in 2012 by the
ATLAS detector operating at the Large Hadron Collider. No
events are observed in any of the signal regions, and limits
are set on model parameters within supersymmetric scenarios
involving R-parity violation, split supersymmetry, and gauge
mediation. In some of the search channels, the trigger and
search strategy are based only on the decay products of
individual long-lived particles, irrespective of the rest of
the event. In these cases, the provided limits can easily be
reinterpreted in different scenarios.},
Doi = {10.1103/PhysRevD.92.072004},
Key = {fds313606}
}
@article{fds307961,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Alvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Aoki, M and Apollinari, G and Apresyan, A and Arisawa,
T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar,
F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bar-Shalom, S and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Bednar, P and Behari, S and Bellettini, G and Bellinger,
J and Belloni, A and Benjamin, D and Beretvas, A and Beringer, J and Berry,
T and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
S and Deisher, A and De Lentdecker and G and De Lorenzo and G and Dell'orso,
M and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent,
PF and Di Giovanni and GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan,
G and Forrest, R and Forrester, S and Franklin, M and Freeman, JC and Furic, I and Gallinaro, M and Galyardt, J and Garberson, F and Garcia,
JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Giagu, S and Giakoumopolou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta, M and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Hamilton, A and Han, B-Y and Han, JY and Handler, R and Happacher, F and Hara, K and Hare, D and Hare,
M and Harper, S and Harr, RF and Harris, RM and Hartz, M and Hatakeyama, K and Hauser, J and Hays, C and Heck, M and Heijboer, A and Heinemann, B and Heinrich, J and Henderson, C and Herndon, M and Heuser, J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker,
A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Huston, J and Incandela, J and Introzzi, G and Iori, M and Ivanov, A and Iyutin, B and James, E and Jayatilaka, B and Jeans, D and Jeon, EJ and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun,
SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato,
Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim,
YK and Kimura, N and Kirsch, L and Klimenko, S and Klute, M and Knuteson,
B and Ko, BR and Koay, SA and Kondo, K and Kong, DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kraus, J and Kreps, M and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhlmann, SE and Kuhr, T and Kulkarni, NP and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, J and Lee, YJ and Lee, SW and Lefèvre, R and Leonardo, N and Leone,
S and Levy, S and Lewis, JD and Lin, C and Lin, CS and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lu, R-S and Lucchesi, D and Lueck, J and Luci, C and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen,
D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic,
P and Malde, S and Malik, S and Manca, G and Manousakis, A and Margaroli,
F and Marino, C and Marino, CP and Martin, A and Martin, M and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and Miao, T and Miladinovic, N and Miles, J and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, M and Movilla
Fernandez, P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Oldeman, R and Orava, R and Osterberg, K and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rajaraman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Reisert, B and Rekovic, V and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Saarikko, H and Safonov, A and Sakumoto, WK and Salamanna, G and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz,
T and Scodellaro, L and Scott, AL and Scribano, A and Scuri, F and Sedov,
A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sfyria, A and Shalhout, SZ and Shapiro, MD and Shears, T and Shepard,
PF and Sherman, D and Shimojima, M and Shochet, M and Shon, Y and Shreyber,
I and Sidoti, A and Sinervo, P and Sisakyan, A},
Title = {Search for maximal flavor violating scalars in same-charge
lepton pairs in pp collisions at sqrt[s]=1.96
TeV.},
Journal = {Physical review letters},
Volume = {102},
Number = {4},
Pages = {041801},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.102.041801},
Abstract = {Models of maximal flavor violation (MxFV) in elementary
particle physics may contain at least one new scalar SU(2)
doublet field Phi(FV)=(eta(0),eta(+)) that couples the first
and third generation quarks (q_(1), q_(3)) via a Lagrangian
term L(FV)=xi(13)Phi(FV)q(1)q(3). These models have a
distinctive signature of same-charge top-quark pairs and
evade flavor-changing limits from meson mixing measurements.
Data corresponding to 2 fb(-1) collected by the Collider
Dectector at Fermilab II detector in pp[over ] collisions at
sqrt[s]=1.96 TeV are analyzed for evidence of the MxFV
signature. For a neutral scalar eta(0) with m_(eta;(0))=200
GeV/c(2) and coupling xi(13)=1, approximately 11 signal
events are expected over a background of 2.1+/-1.8 events.
Three events are observed in the data, consistent with
background expectations, and limits are set on the coupling
xi(13) for m(eta(0)=180-300 GeV/c(2).},
Doi = {10.1103/physrevlett.102.041801},
Key = {fds307961}
}
@article{fds317297,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black, CW and Black, JE and Black,
KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato,
E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt,
AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J},
Title = {Search for metastable heavy charged particles with large
ionisation energy loss in pp collisions at [Formula:
see text] TeV using the ATLAS experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {9},
Pages = {407},
Year = {2015},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3609-0},
Abstract = {Many extensions of the Standard Model predict the existence
of charged heavy long-lived particles, such as
<i>R</i>-hadrons or charginos. These particles, if produced
at the Large Hadron Collider, should be moving
non-relativistically and are therefore identifiable through
the measurement of an anomalously large specific energy loss
in the ATLAS pixel detector. Measuring heavy long-lived
particles through their track parameters in the vicinity of
the interaction vertex provides sensitivity to metastable
particles with lifetimes from 0.6 ns to 30 ns. A search
for such particles with the ATLAS detector at the Large
Hadron Collider is presented, based on a data sample
corresponding to an integrated luminosity of [Formula: see
text] fb[Formula: see text] of <i>pp</i> collisions at
[Formula: see text] TeV. No significant deviation from the
Standard Model background expectation is observed, and
lifetime-dependent upper limits on <i>R</i>-hadrons and
chargino production are set. Gluino <i>R</i>-hadrons with
10 ns lifetime and masses up to 1185 GeV are excluded at
95 [Formula: see text] confidence level, and so are
charginos with 15 ns lifetime and masses up to
482 GeV.},
Doi = {10.1140/epjc/s10052-015-3609-0},
Key = {fds317297}
}
@article{fds321124,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for metastable heavy charged particles with large
ionization energy loss in pp collisions at s =13 TeV using
the ATLAS experiment},
Journal = {Physical Review D},
Volume = {93},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.93.112015},
Abstract = {This paper presents a search for massive charged long-lived
particles produced in pp collisions at s=13 TeV at the LHC
using the ATLAS experiment. The data set used corresponds to
an integrated luminosity of 3.2 fb-1. Many extensions of the
Standard Model predict the existence of massive charged
long-lived particles, such as R-hadrons. These massive
particles are expected to be produced with a velocity
significantly below the speed of light, and therefore to
have a specific ionization higher than any Standard Model
particle of unit charge at high momenta. The Pixel subsystem
of the ATLAS detector is used to measure the ionization
energy loss of reconstructed charged particles and to search
for such highly ionizing particles. The search presented
here has much greater sensitivity than a similar search
performed using the ATLAS detector in the s=8 TeV data set,
thanks to the increase in expected signal cross section due
to the higher center-of-mass energy of collisions, to an
upgraded detector with a new silicon layer close to the
interaction point, and to analysis improvements. No
significant deviation from Standard Model background
expectations is observed, and lifetime-dependent upper
limits on R-hadron production cross sections and masses are
set. Gluino R-hadrons with lifetimes above 0.4 ns and
decaying to qq plus a 100 GeV neutralino are excluded at the
95% confidence level, with lower mass limit ranging between
740 and 1590 GeV. In the case of stable R-hadrons the lower
mass limit at the 95% confidence level is 1570
GeV.},
Doi = {10.1103/PhysRevD.93.112015},
Key = {fds321124}
}
@article{fds310370,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for microscopic black holes and string balls in final
states with leptons and jets with the ATLAS detector at √s
= 8 TeV},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {8},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP08(2014)103},
Abstract = {A search for an excess of events with multiple high
transverse momentum objects including charged leptons and
jets is presented, using 20.3 fb -1 of proton-proton
collision data recorded by the ATLAS detector at the Large
Hadron Collider in 2012 at a centre-of-mass energy of √s =
8 TeV. No excess of events beyond Standard Model
expectations is observed. Using extra-dimensional models for
black hole and string ball production and decay, exclusion
contours are determined as a function of the mass threshold
for production and the fundamental gravity scale for two,
four and six extra dimensions. For six extra dimensions,
mass thresholds of 4.8-6.2 TeV are excluded at 95 %
confidence level, depending on the fundamental gravity scale
and model assumptions. Upper limits on the fiducial
cross-sections for non-Standard Model production of these
final states are set. [Figure not available: see fulltext.]
© 2014 The Author(s).},
Doi = {10.1007/JHEP08(2014)103},
Key = {fds310370}
}
@article{fds307572,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for microscopic black holes in a like-sign dimuon
final state using large track multiplicity with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.88.072001},
Abstract = {A search is presented for microscopic black holes in a
like-sign dimuon final state in proton-proton collisions at
√s=8 TeV. The data were collected with the ATLAS detector
at the Large Hadron Collider in 2012 and correspond to an
integrated luminosity of 20.3 fb-1. Using a high track
multiplicity requirement, 0.6±0.2 background events from
Standard Model processes are predicted and none observed.
This result is interpreted in the context of low-scale
gravity models and 95% C.L. lower limits on microscopic
black hole masses are set for different model assumptions.
© 2013 CERN. Published by the American Physical Society
under the terms of the Creative Commons Attribution 3.0
License. Further distribution of this work must maintain
attribution to the author(s) and the published article's
title, journal citation, and DOI.},
Doi = {10.1103/PhysRevD.88.072001},
Key = {fds307572}
}
@article{fds332352,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Bolton,
TA and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and De,
K and Jong, SJ and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot,
L},
Title = {Search for minimal supergravity in single-electron events
with jets and large missing transverse energy in [Formula
Presented] collisions at [Formula Presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {66},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.66.112001},
Abstract = {We describe a search for evidence of minimal supergravity
(MSUGRA) in [Formula Presented] of data collected with the
DØ detector at the Fermilab Tevatron [Formula Presented]
collider at [Formula Presented] Events with a single
electron, four or more jets, and large missing transverse
energy were used in this search. The major backgrounds are
from [Formula Presented] misidentified multijet, [Formula
Presented] and [Formula Presented] production. We observe no
excess above the expected number of background events in our
data. A new limit in terms of MSUGRA model parameters is
obtained. © 2002 The American Physical Society.},
Doi = {10.1103/PhysRevD.66.112001},
Key = {fds332352}
}
@article{fds321075,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Baarreiro Guimrães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Billoud, TRV and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
Title = {Search for minimal supersymmetric standard model Higgs
Bosons H / A and for a [Formula: see text] boson in the
[Formula: see text] final state produced in pp collisions at
[Formula: see text] TeV with the ATLAS detector.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {11},
Pages = {585},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4400-6},
Abstract = {A search for neutral Higgs bosons of the minimal
supersymmetric standard model (MSSM) and for a heavneutral
[Formula: see text] boson is performed using a data sample
corresponding to an integrated luminosity of
3.2 fb[Formula: see text] from proton-proton collisions at
[Formula: see text] [Formula: see text] recorded by the
ATLAS detector at the LHC. The heavy resonance is assumed to
decay to a [Formula: see text] pair with at least one
[Formula: see text] lepton decaying to final states with
hadrons and a neutrino. The search is performed in the mass
range of 0.2-1.2 [Formula: see text] for the MSSM neutral
Higgs bosons and 0.5-2.5 [Formula: see text] for the
heavy neutral [Formula: see text] boson. The data are in
good agreement with the background predicted by the Standard
Model. The results are interpreted in MSSM and [Formula: see
text] benchmark scenarios. The most stringent constraints on
the MSSM [Formula: see text]-[Formula: see text] space
exclude at 95 % confidence level (CL) [Formula: see text]
for [Formula: see text] [Formula: see text] in the
[Formula: see text] MSSM scenario. For the Sequential
Standard Model, a [Formula: see text] mass up to
1.90 [Formula: see text] is excluded at 95 % CL and
masses up to 1.82-2.17 [Formula: see text] are excluded
for a [Formula: see text] of the strong flavour
model.},
Doi = {10.1140/epjc/s10052-016-4400-6},
Key = {fds321075}
}
@article{fds307996,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D},
Title = {Search for narrow resonances lighter than Υ
mesons},
Journal = {European Physical Journal C},
Volume = {62},
Number = {2},
Pages = {319-326},
Publisher = {Springer Nature},
Year = {2009},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-009-1057-4},
Abstract = {We report a search for narrow resonances, produced in p p̄
collisions at √ s=1.96 TeV, that decay into muon pairs
with invariant mass between 6.3 and 9.0 GeV/c 2. The data,
collected with the CDF II detector at the Fermilab Tevatron
collider, correspond to an integrated luminosity of 630 pb
-1. We use the dimuon invariant mass distribution to set 90%
upper credible limits of about 1% to the ratio of the
production cross section times muonic branching fraction of
possible narrow resonances to that of the Υ(1S) meson. ©
2009 Springer-Verlag.},
Doi = {10.1140/epjc/s10052-009-1057-4},
Key = {fds307996}
}
@article{fds307670,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Alexeev, GD and Alkhazov, G and Alton, A and Lvarez
González, B and Alverson, G and Amerio, S and Amidei, D and Anastassov,
A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa,
T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins,
S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Bose, T and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown, D and Brown, J and Brucken, E and Budagov, J and Bu, XB and Budd, HS and Buehler,
M and Buescher, V and Bunichev, V and Burdin, S},
Title = {Search for neutral Higgs bosons in events with multiple
bottom quarks at the Tevatron},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.86.091101},
Abstract = {The combination of searches performed by the CDF and D0
collaborations at the Fermilab Tevatron Collider for neutral
Higgs bosons produced in association with b quarks is
reported. The data, corresponding to 2.6fb -1 of integrated
luminosity at CDF and 5.2fb -1 at D0, have been collected in
final states containing three or more b jets. Upper limits
are set on the cross section multiplied by the branching
ratio varying between 44 pb and 0.7 pb in the Higgs boson
mass range 90 to 300 GeV, assuming production of a narrow
scalar boson. Significant enhancements to the production of
Higgs bosons can be found in theories beyond the standard
model, for example, in supersymmetry. The results are
interpreted as upper limits in the parameter space of the
minimal supersymmetric standard model in a benchmark
scenario favoring this decay mode. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.091101},
Key = {fds307670}
}
@article{fds308105,
Author = {Abulencia, A and Acosta, D and Adelman, J and Affolder, T and Akimoto,
T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov,
A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arguin, J-F and Arisawa, T and Artikov, A and Ashmanskas, W and Attal,
A and Azfar, F and Azzi-Bacchetta, P and Azzurri, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Bartsch, V and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Beringer,
J and Berry, T and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Boveia, A and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi, R and Carron, S and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chapman,
J and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chu, PH and Chuang, SH and Chung, K and Chung, WH and Chung, YS and Ciljak, M and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Coca, M and Connolly, A and Convery, ME and Conway, J and Cooper, B and Copic, K and Cordelli, M and Cortiana, G and Cruz, A and Cuevas, J and Culbertson, R and Cyr, D and Daronco, S and D'Auria, S and D'onofrio, M and Dagenhart, D and de Barbaro, P and De Cecco and S and Deisher, A and De Lentdecker and G and Dell'Orso, M and Demers, S and Demortier, L and Deng, J and Deninno, M and De Pedis and D and Derwent, PF and Dionisi, C and Dittmann, J and Dituro,
P and Dörr, C and Dominguez, A and Donati, S and Donega, M and Dong, P and Donini, J and Dorigo, T and Dube, S and Ebina, K and Efron, J and Ehlers,
J and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, I and Fedorko, WT and Feild, RG and Feindt,
M and Fernandez, JP and Field, R and Flanagan, G and Flores-Castillo,
LR and Foland, A and Forrester, S and Foster, GW and Franklin, M and Freeman, JC and Fujii, Y and Furic, I and Gajjar, A and Gallinaro, M and Galyardt, J and Garcia, JE and Garcia Sciveres and M and Garfinkel, AF and Gay, C and Gerberich, H and Gerchtein, E and Gerdes, D and Giagu, S and Giannetti, P and Gibson, A and Gibson, K and Ginsburg, C and Giolo, K and Giordani, M and Giunta, M and Giurgiu, G and Glagolev, V and Glenzinski,
D and Gold, M and Goldschmidt, N and Goldstein, J and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Gotra, Y and Goulianos, K and Gresele, A and Griffiths,
M and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes
da Costa, J and Haber, C and Hahn, SR and Hahn, K and Halkiadakis, E and Hamilton, A and Han, B-Y and Handler, R and Happacher, F and Hara, K and Hare, M and Harper, S and Harr, RF and Harris, RM and Hatakeyama, K and Hauser, J and Hays, C and Hayward, H and Heijboer, A and Heinemann, B and Heinrich, J and Hennecke, M and Herndon, M and Heuser, J and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Holloway, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Huston, J and Ikado, K and Incandela, J and Introzzi, G and Iori, M and Ishizawa, Y and Ivanov, A and Iyutin, B and James, E and Jang, D and Jayatilaka, B and Jeans, D and Jensen, H and Jeon, EJ and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Kang, J and Karagoz-Unel, M and Karchin, PE and Kato, Y and Kemp, Y and Kephart, R and Kerzel, U and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, MS and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirsch, L and Klimenko, S and Klute, M and Knuteson, B and Ko, BR and Kobayashi, H and Kondo, K and Kong,
DJ and Konigsberg, J and Kordas, K and Korytov, A and Kotwal, AV and Kovalev, A and Kraus, J and Kravchenko, I and Kreps, M and Kreymer, A and Kroll, J and Krumnack, N and Kruse, M and Krutelyov, V and Kuhlmann, SE and Kusakabe, Y and Kwang, S and Laasanen, AT and Lai, S and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecci, C and Lecompte, T and Lee, J and Lee, SW and Lefèvre, R and Leonardo, N and Leone, S and Levy, S and Lewis,
JD and Li, K and Lin, C and Lin, CS and Lindgren, M and Lipeles, E and Liss,
TM and Lister, A and Litvintsev, DO and Liu, T and Liu, Y and Lockyer, NS and Loginov, A and Loreti, M and Loverre, P and Lu, R-S and Lucchesi, D and Lujan, P and Lukens, P and Lungu, G and Lyons, L and Lys, J and Lysak, R and Lytken, E and Mack, P and Macqueen, D and Madrak, R and Maeshima, K and Maksimovic, P and Manca, G and Margaroli, F and Marginean, R and Marino,
C and Martin, A and Martin, M and Martin, V and Martínez, M and Maruyama,
T and Matsunaga, H and Mattson, ME and Mazini, R and Mazzanti, P and McFarland, KS and McGivern, D and McIntyre, P and McNamara, P and McNulty, R and Mehta, A and Menzemer, S and Menzione, A and Merkel, P and Mesropian, C and Messina, A and von der Mey, M and Miao, T and Miladinovic, N and Miles, J and Miller, R and Miller, JS and Mills, C and Milnik, M and Miquel, R and Miscetti, S and Mitselmakher, G and Miyamoto, A and Moggi, N and Mohr, B and Moore, R and Morello, M and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Mulhearn, M and Muller, T and Mumford, R and Murat, P and Nachtman, J and Nahn, S and Nakano, I and Napier, A and Naumov, D and Necula, V and Neu, C and Neubauer, MS and Nielsen, J and Nigmanov, T and Nodulman, L and Norniella, O and Ogawa, T and Oh, SH and Oh, YD and Okusawa, T and Oldeman,
R and Orava, R and Osterberg, K and Pagliarone, C and Palencia, E and Paoletti, R and Papadimitriou, V and Papikonomou, A and Paramonov,
AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Piedra, J and Pitts, K and Plager, C and Pondrom, L and Pope, G and Portell, X and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos, F and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Rakitin, A and Rappoccio, S and Ratnikov, F and Reisert, B and Rekovic, V and van Remortel, N and Renton, P and Rescigno, M and Richter, S and Rimondi, F and Rinnert, K and Ristori, L and Robertson, WJ and Robson, A and Rodrigo, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Rott, C and Ruiz, A and Russ, J and Rusu, V and Ryan, D and Saarikko, H and Sabik, S and Safonov,
A and Sakumoto, WK and Salamanna, G and Salto, O and Saltzberg, D and Sanchez, C and Santi, L and Sarkar, S and Sato, K and Savard, P and Savoy-Navarro, A and Scheidle, T and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scott,
AL and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Semeria, F and Sexton-Kennedy, L and Sfiligoi,
I},
Title = {Search for neutral Higgs bosons of the minimal
supersymmetric standard model decaying to tau pairs in pp
collisions at square root of s = 1.96 TeV.},
Journal = {Physical review letters},
Volume = {96},
Number = {1},
Pages = {011802},
Year = {2006},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.96.011802},
Abstract = {We present a search for neutral supersymmetric Higgs bosons
decaying to tau pairs produced in pp collisions at square
root of s = 1.96 TeV. The data, corresponding to 310 pb(-1)
integrated luminosity, were collected with the Collider
Detector at Fermilab in run II of the Tevatron. No
significant excess above the standard model backgrounds is
observed. We set exclusion limits on the production cross
section times branching fraction to tau pairs for Higgs
boson masses in the range from 90 to 250
GeV/c2.},
Doi = {10.1103/physrevlett.96.011802},
Key = {fds308105}
}
@article{fds310346,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for neutral Higgs bosons of the minimal
supersymmetric standard model in pp collisions at vs= 8TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {11},
Pages = {1-47},
Publisher = {Springer Nature},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2014)056},
Abstract = {Abstract: A search for the neutral Higgs bosons predicted by
the Minimal Supersymmetric Standard Model (MSSM) is
reported. The analysis is performed on data from
proton-proton collisions at a centre-of-mass energy of 8 TeV
collected with the ATLAS detector at the Large Hadron
Collider. The samples used for this search were collected in
2012 and correspond to integrated luminosities in the range
19.5-20.3 fb−1. The MSSM Higgs bosons are searched for in
the τ τ final state. No significant excess over the
expected background is observed, and exclusion limits are
derived for the production cross section times branching
fraction of a scalar particle as a function of its mass. The
results are also interpreted in the MSSM parameter space for
various benchmark scenarios.},
Doi = {10.1007/JHEP11(2014)056},
Key = {fds310346}
}
@article{fds307862,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Search for neutral MSSM Higgs bosons decaying to
τ+τ- pairs in proton-proton
collisions at s=7 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {705},
Number = {3},
Pages = {174-192},
Publisher = {Elsevier BV},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2011.10.001},
Abstract = {A search for neutral Higgs bosons decaying to pairs of τ
leptons with the ATLAS detector at the LHC is presented. The
analysis is based on proton-proton collisions at a
center-of-mass energy of 7 TeV, recorded in 2010 and
corresponding to an integrated luminosity of 36 pb-1. After
signal selection, 276 events are observed in this data
sample. The observed number of events is consistent with the
total expected background of 269±36 events. Exclusion
limits at the 95% confidence level are derived for the
production cross section of a generic Higgs boson φ as a
function of the Higgs boson mass and for A/H/h production in
the Minimal Supersymmetric Standard Model (MSSM) as a
function of the parameters mA and tanβ. © 2011
CERN.},
Doi = {10.1016/j.physletb.2011.10.001},
Key = {fds307862}
}
@article{fds307834,
Author = {Aaltonen, TEA},
Title = {Search for New ${T}^\prime$ Particles in Final States with
Large Jet Multiplicities and Missing Transverse Energy in
$p\overline{p}$ Collisions at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {19},
Pages = {191803},
Publisher = {American Physical Society},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.191803},
Abstract = {We present a search for a new particle T' decaying to a top
quark via T' → t + X, where X goes undetected. We use a
data sample corresponding to 5.7 fb(-1) of integrated
luminosity of p p collisions with sqrt[s] = 1.96 TeV,
collected at Fermilab Tevatron by the CDF II detector. Our
search for pair production of T' is focused on the hadronic
decay channel, pp → T'T' → tt + XX → bqq b qq + XX. We
interpret our results in terms of a model where T' is an
exotic fourth generation quark and X is a dark matter
particle. The data are consistent with standard model
expectations. We set a limit on the generic production of
T'T' → tt + XX, excluding the fourth generation exotic
quarks T' at 95% confidence level up to m(T') = 400 GeV/c(2)
for m(X) ≤ 70 GeV/c(2).},
Doi = {10.1103/PhysRevLett.107.191803},
Key = {fds307834}
}
@article{fds307910,
Author = {Aaltonen, and T, and others},
Title = {Search for New Bottomlike Quark Pair Decays $Q\bar{Q} \to
(tW^\mp)(\bar{t}W^\pm)$ in Same-Charge Dilepton
Events},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {9},
Pages = {091801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.091801},
Abstract = {http://arxiv.org/abs/0912.1057},
Doi = {10.1103/PhysRevLett.104.091801},
Key = {fds307910}
}
@article{fds307929,
Author = {Aaltonen, and T, and others},
Title = {Search for New Color-Octet Vector Particle Decaying to $t
\bar{t}$ in $p \bar{p}$ Collisions at $\sqrt{s}=1.96$
TeV},
Journal = {Phys. Lett.},
Volume = {B691},
Number = {4},
Pages = {183-190},
Publisher = {Elsevier BV},
Year = {2010},
url = {http://dx.doi.org/10.1016/j.physletb.2010.06.036},
Abstract = {http://arxiv.org/abs/0911.3112},
Doi = {10.1016/j.physletb.2010.06.036},
Key = {fds307929}
}
@article{fds307840,
Author = {Aaltonen, and T, and al, E},
Title = {Search for New Dielectron Resonances and {Randall-Sundrum}
Gravitons at the {Collider Detector at Fermilab}},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {5},
Pages = {051801},
Publisher = {American Physical Society},
Year = {2011},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.051801},
Abstract = {A search for new dielectron-mass resonances using data
recorded by the CDF II detector and corresponding to an
integrated luminosity of 5.7 fb(-1) is presented. No
significant excess over the expected standard model
prediction is observed. In this data set, an event with the
highest dielectron mass ever observed (960 GeV/c(2))
was recorded. The results are interpreted in the
Randall-Sundrum (RS) model. Combined with the
5.4 fb(-1) diphoton analysis, the RS-graviton
lower-mass limit for the coupling k/M¯(Pl)=0.1 is
1058 GeV/c(2), making it the strongest limit to
date.},
Doi = {10.1103/PhysRevLett.107.051801},
Key = {fds307840}
}
@article{fds307884,
Author = {Aaltonen, and T, and al, E},
Title = {Search for new heavy particles decaying to ${ZZ}\rightarrow
llll$, $lljj$ in $p\overline{p}$ collisions at
$\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {11},
Pages = {112008},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.112008},
Abstract = {We report on a search for anomalous production of Z boson
pairs through a massive resonance decay in data
corresponding to 2.5-2.9fb-1 of integrated luminosity in
pp̄ collisions at √s=1.96TeV using the CDF II detector at
the Fermilab Tevatron. This analysis, with more data and
channels where the Z bosons decay to muons or jets,
supersedes the 1.1fb-1 four-electron channel result
previously published by CDF. In order to maintain high
efficiency for muons, we use a new forward tracking
algorithm and muon identification requirements optimized for
these high signal-to-background channels. Predicting the
dominant backgrounds in each channel entirely from sideband
data samples, we observe four-body invariant mass spectra
above 300GeV/c2 that are consistent with background. We set
limits using the acceptance for a massive graviton resonance
that are 7-20 times stronger than the previously published
direct limits on resonant ZZ diboson production. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.112008},
Key = {fds307884}
}
@article{fds351559,
Author = {Abulencia, and A, and others},
Title = {Search for new high mass particles decaying to lepton pairs
in p anti-p collisions at s**(1/2) = 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {95},
Number = {25},
Pages = {252001},
Year = {2005},
url = {http://dx.doi.org/10.1103/physrevlett.95.252001},
Abstract = {A search for new particles (X) that decay to electron or
muon pairs has been performed using approximately 200 pb-1
of pp-bar collision data at sqrt[s]=1.96 TeV collected by
the CDF II experiment at the Fermilab Tevatron. Limits on
sigma (pp-bar-->X)BR(X-->ll) are presented as a function of
dilepton invariant mass mll>150 GeV/c2, for different spin
hypotheses (0, 1, or 2). The limits are approximately 25 fb
for mll>600 GeV/c2. Lower mass bounds for X from
representative models beyond the standard model including
heavy neutral gauge bosons are presented.},
Doi = {10.1103/physrevlett.95.252001},
Key = {fds351559}
}
@article{fds356734,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for new high-mass phenomena in the dilepton final
state using 36 fb−1 of proton-proton collision
data at √s=13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {10},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2017)182},
Abstract = {A search is conducted for new resonant and non-resonant
high-mass phenomena in dielectron and dimuon final states.
The search uses 36.1 fb−1 of proton-proton collision data,
collected at s=13 TeV by the ATLAS experiment at the LHC in
2015 and 2016. No significant deviation from the Standard
Model prediction is observed. Upper limits at 95%
credibility level are set on the cross-section times
branching ratio for resonances decaying into dileptons,
which are converted to lower limits on the resonance mass,
up to 4.1 TeV for the E6-motivated Zχ′. Lower limits on
the qqℓℓ contact interaction scale are set between 2.4
TeV and 40 TeV, depending on the model.},
Doi = {10.1007/JHEP10(2017)182},
Key = {fds356734}
}
@article{fds353083,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
Title = {Search for new non-resonant phenomena in high-mass dilepton
final states with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2020)005},
Abstract = {A search for new physics with non-resonant signals in
dielectron and dimuon final states in the mass range above 2
TeV is presented. This is the first search for non-resonant
signals in dilepton final states at the LHC to use a
background estimate from the data. The data, corresponding
to an integrated luminosity of 139 fb−1, were recorded by
the ATLAS experiment in proton-proton collisions at a
center-of-mass energy of s = 13 TeV during Run 2 of the
Large Hadron Collider. The benchmark signal signature is a
two-quark and two-lepton contact interaction, which would
enhance the dilepton event rate at the TeV mass scale. To
model the contribution from background processes a
functional form is fit to the dilepton invariant-mass
spectra in data in a mass region below the region of
interest. It is then extrapolated to a high-mass signal
region to obtain the expected background there. No
significant deviation from the expected background is
observed in the data. Upper limits at 95% CL on the number
of events and the visible cross-section times branching
fraction for processes involving new physics are provided.
Observed (expected) 95% CL lower limits on the contact
interaction energy scale reach 35.8 (37.6) TeV. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP11(2020)005},
Key = {fds353083}
}
@article{fds307981,
Author = {Aaltonen, T and others},
Title = {Search for new particles decaying into dijets in
proton-antiproton collisions at sqrt(s) = 1.96
TeV},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {11},
Pages = {112002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112002},
Abstract = {We present a search for new particles which produce narrow
two-jet (dijet) resonances using proton-antiproton collision
data corresponding to an integrated luminosity of 1.13fb-1
collected with the CDFA II detector. The measured dijet mass
spectrum is found to be consistent with next-to-leading-order
perturbative QCD predictions, and no significant evidence of
new particles is found. We set upper limits at the 95%
confidence level on cross sections times the branching
fraction for the production of new particles decaying into
dijets with both jets having a rapidity magnitude |y| <1.
These limits are used to determine the mass exclusions for
the excited quark, axigluon, flavor-universal coloron, E6
diquark, color-octet techni-ρ, W′, and Z′. © 2009 The
American Physical Society.},
Doi = {10.1103/PhysRevD.79.112002},
Key = {fds307981}
}
@article{fds307726,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli,
EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani,
G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW},
Title = {Search for new particles decaying to ZZ using final states
with leptons and jets with the ATLAS detector in √s=7 TeV
proton-proton collisions},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {712},
Number = {4-5},
Pages = {331-350},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.05.020},
Abstract = {A search is presented for a narrow resonance decaying to a
pair of Z bosons using data corresponding to 1.02fb-1 of
integrated luminosity collected by the ATLAS experiment from
pp collisions at √s=7TeV. Events containing either four
charged leptons (ℓℓℓℓ) or two charged leptons and
two jets (ℓℓjj) are analyzed and found to be consistent
with the Standard Model background expectation. Lower limits
on a resonance mass are set using the Randall-Sundrum (RS1)
graviton model as a benchmark. Using both ℓℓℓℓ and
ℓℓjj events, an RS1 graviton with k/m-pl=0.1 and mass
between 325 and 845 GeV is excluded at 95% confidence level.
In addition, the ℓℓℓℓ events are used to set a
model-independent fiducial cross section limit of
σfid(pp→X→ZZ)<0.92pb at 95% confidence level for any
new sources of ZZ production with mZZ greater than 300 GeV.
© 2012 CERN.},
Doi = {10.1016/j.physletb.2012.05.020},
Key = {fds307726}
}
@article{fds317302,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for new particles in events with one lepton and
missing transverse momentum in pp collisions at √s = 8 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Pages = {1-42},
Publisher = {Springer Nature},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2014)037},
Abstract = {This paper presents a search for new particles in events
with one lepton (electron or muon) and missing transverse
momentum using 20.3 fb−1 of proton-proton collision data
at √s = 8 TeV recorded by the ATLAS experiment at the
Large Hadron Collider. No significant excess beyond Standard
Model expectations is observed. A W ′ with Sequential
Standard Model couplings is excluded at the 95% confidence
level for masses up to 3.24 TeV. Excited chiral bosons (W*)
with equivalent coupling strengths are excluded for masses
up to 3.21 TeV. In the framework of an effective field
theory limits are also set on the dark matter-nucleon
scattering cross-section as well as the mass scale M* of the
unknown mediating interaction for dark matter pair
production in association with a leptonically decaying
W.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP09(2014)037},
Key = {fds317302}
}
@article{fds308067,
Author = {Aaltonen, and T, and others},
Title = {Search for New Particles Leading to $Z +$ jets Final States
in $p \bar{p}$ Collisions at $\sqrt{s}$ =
1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D76},
Number = {7},
Pages = {072006},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.76.072006},
Abstract = {We present the results of a search for new particles that
lead to a Z boson plus jets in p[overline p] collisions at
sqrt(s)=1.96 TeV using the Collider Detector at Fermilab
(CDF II). A data sample with a luminosity of 1.06 fb-1
collected using Z boson decays to ee and µµ is used. We
describe a completely data-based method to predict the
dominant background from standard model Z+jet events. This
method can be similarly applied to other analyses requiring
background predictions in multijet environments, as shown
when validating the method by predicting the background from
W+jets in t[overline t] production. No significant excess
above the background prediction is observed, and a limit is
set using a fourth generation quark model to quantify the
acceptance. Assuming BR(b[prime]-->bZ)=100\% and using a
leading-order calculation of the b[prime] cross section,
b[prime] quark masses below 268 GeV/c2 are excluded at 95%
confidence level.},
Doi = {10.1103/PhysRevD.76.072006},
Key = {fds308067}
}
@article{fds356737,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for new phenomena in a lepton plus high jet
multiplicity final state with the ATLAS experiment using
√s=13 TeV proton-proton collision data},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {9},
Year = {2017},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2017)088},
Abstract = {A search for new phenomena in final states characterized by
high jet multiplicity, an isolated lepton (electron or muon)
and either zero or at least three b-tagged jets is
presented. The search uses 36.1 fb−1 of s=13 TeV
proton-proton collision data collected by the ATLAS
experiment at the Large Hadron Collider in 2015 and 2016.
The dominant sources of background are estimated using
parameterized extrapolations, based on observables at medium
jet multiplicity, to predict the b-tagged jet multiplicity
distribution at the higher jet multiplicities used in the
search. No significant excess over the Standard Model
expectation is observed and 95% confidence-level limits are
extracted constraining four simplified models of
R-parity-violating supersymmetry that feature either gluino
or top-squark pair production. The exclusion limits reach as
high as 2.1 TeV in gluino mass and 1.2 TeV in top-squark
mass in the models considered. In addition, an upper limit
is set on the cross-section for Standard Model tt¯ tt¯
production of 60 fb (6.5 × the Standard Model prediction)
at 95% confidence level. Finally, model-independent limits
are set on the contribution from new phenomena to the
signal-region yields.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP09(2017)088},
Key = {fds356737}
}
@article{fds325794,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
Title = {Search for new phenomena in different-flavour high-mass
dilepton final states in pp collisions at [Formula:
see text] Tev with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {541},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4385-1},
Abstract = {A search is performed for a heavy particle decaying into
different flavour dilepton pairs ([Formula: see text],
[Formula: see text] or [Formula: see text]), using
3.2 fb[Formula: see text] of proton-proton collision data
at [Formula: see text] TeV collected in 2015 by the ATLAS
detector at the Large Hadron Collider. No excess over the
Standard Model prediction is observed. Limits at the 95 %
credibility level are set on the mass of a [Formula: see
text] boson with lepton-flavour-violating couplings at 3.0,
2.7 and 2.6 TeV, and on the mass of a supersymmetric
[Formula: see text] sneutrino with <i>R</i>-parity-violating
couplings at 2.3, 2.2 and 1.9 TeV, for [Formula: see text],
[Formula: see text] and [Formula: see text] final states,
respectively. The results are also interpreted as limits on
the threshold mass for quantum black hole
production.},
Doi = {10.1140/epjc/s10052-016-4385-1},
Key = {fds325794}
}
@article{fds310278,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA},
Title = {Search for New Phenomena in Dijet Angular Distributions in
Proton-Proton Collisions at sqrt[s]=8 TeV Measured with the
ATLAS Detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {22},
Pages = {221802},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.114.221802},
Abstract = {A search for new phenomena in LHC proton-proton collisions
at a center-of-mass energy of sqrt[s]=8 TeV was performed
with the ATLAS detector using an integrated luminosity of
17.3 fb^{-1}. The angular distributions are studied in
events with at least two jets; the highest dijet mass
observed is 5.5 TeV. All angular distributions are
consistent with the predictions of the standard model. In a
benchmark model of quark contact interactions, a
compositeness scale below 8.1 TeV in a destructive
interference scenario and 12.0 TeV in a constructive
interference scenario is excluded at 95% C.L.; median
expected limits are 8.9 TeV for the destructive interference
scenario and 14.1 TeV for the constructive interference
scenario.},
Doi = {10.1103/physrevlett.114.221802},
Key = {fds310278}
}
@article{fds356740,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Search for new phenomena in dijet events using 37 fb-1 of pp
collision data collected at √s=13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {96},
Number = {5},
Year = {2017},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.96.052004},
Abstract = {Dijet events are studied in the proton-proton collision data
set recorded at s=13 TeV with the ATLAS detector at the
Large Hadron Collider in 2015 and 2016, corresponding to
integrated luminosities of 3.5 fb-1 and 33.5 fb-1
respectively. Invariant mass and angular distributions are
compared to background predictions and no significant
deviation is observed. For resonance searches, a new method
for fitting the background component of the invariant mass
distribution is employed. The data set is then used to set
upper limits at a 95% confidence level on a range of new
physics scenarios. Excited quarks with masses below 6.0 TeV
are excluded, and limits are set on quantum black holes,
heavy W′ bosons, W∗ bosons, and a range of masses and
couplings in a Z′ dark matter mediator model.
Model-independent limits on signals with a Gaussian shape
are also set, using a new approach allowing factorization of
physics and detector effects. From the angular
distributions, a scale of new physics in contact interaction
models is excluded for scenarios with either constructive or
destructive interference. These results represent a
substantial improvement over those obtained previously with
lower integrated luminosity.},
Doi = {10.1103/PhysRevD.96.052004},
Key = {fds356740}
}
@article{fds356775,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O},
Title = {Search for new phenomena in dijet mass and angular
distributions from pp collisions at √s=13 TeV with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {754},
Pages = {302-322},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2016.01.032},
Abstract = {This Letter describes a model-agnostic search for pairs of
jets (dijets) produced by resonant and non-resonant
phenomena beyond the Standard Model in 3.6 fb−1 of
proton–proton collisions with a centre-of-mass energy of
s=13 TeV recorded by the ATLAS detector at the Large Hadron
Collider. The distribution of the invariant mass of the two
leading jets is examined for local excesses above a
data-derived estimate of the smoothly falling prediction of
the Standard Model. The data are also compared to a Monte
Carlo simulation of Standard Model angular distributions
derived from the rapidity of the two jets. No evidence of
anomalous phenomena is observed in the data, which are used
to exclude, at 95% CL, quantum black holes with threshold
masses below 8.3 TeV, 8.1 TeV, or 5.1 TeV in three different
benchmark scenarios; resonance masses below 5.2 TeV for
excited quarks, 2.6 TeV in a W′ model, a range of masses
starting from mZ′=1.5 TeV and couplings from gq=0.2 in a
Z′ model; and contact interactions with a compositeness
scale below 12.0 TeV and 17.5 TeV respectively for
destructive and constructive interference between the new
interaction and QCD processes. These results significantly
extend the ATLAS limits obtained from 8 TeV data.
Gaussian-shaped contributions to the mass distribution are
also excluded if the effective cross-section exceeds values
ranging from approximately 50–300 fb for masses below 2
TeV to 2–20 fb for masses above 4 TeV.},
Doi = {10.1016/j.physletb.2016.01.032},
Key = {fds356775}
}
@article{fds347493,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu,
H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk,
L and Adams, DL and Adelman, J and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa,
JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti,
M and De Mendizabal and JB and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt,
J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de
Renstrom, PAB and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castelli,
A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
LC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Search for new phenomena in events containing a same-flavour
opposite-sign dilepton pair, jets, and large missing
transverse momentum in [Formula: see text] [Formula: see
text][Formula: see text] collisions with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {3},
Pages = {144},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4700-5},
Abstract = {Two searches for new phenomena in final states containing a
same-flavour opposite-sign lepton (electron or muon) pair,
jets, and large missing transverse momentum are presented.
These searches make use of proton-proton collision data,
collected during 2015 and 2016 at a centre-of-mass energy
[Formula: see text] [Formula: see text] by the ATLAS
detector at the large hadron collider, which correspond to
an integrated luminosity of [Formula: see text]. Both
searches target the pair production of supersymmetric
particles, squarks or gluinos, which decay to final states
containing a same-flavour opposite-sign lepton pair via one
of two mechanisms: a leptonically decaying <i>Z</i> boson in
the final state, leading to a peak in the dilepton
invariant-mass distribution around the <i>Z</i> boson mass;
and decays of neutralinos (e.g. [Formula: see text]),
yielding a kinematic endpoint in the dilepton invariant-mass
spectrum. The data are found to be consistent with the
Standard Model expectation. Results are interpreted in
simplified models of gluino-pair (squark-pair) production,
and provide sensitivity to gluinos (squarks) with masses as
large as 1.70 [Formula: see text] (980 [Formula: see
text]).},
Doi = {10.1140/epjc/s10052-017-4700-5},
Key = {fds347493}
}
@article{fds321125,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Search for new phenomena in events with a photon and missing
transverse momentum in pp collisions at √s = 13 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {6},
Pages = {1-41},
Publisher = {Springer Nature},
Year = {2016},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2016)059},
Abstract = {Results of a search for new phenomena in events with an
energetic photon and large missing transverse momentum with
the ATLAS experiment at the Large Hadron Collider are
reported. The data were collected in proton-proton
collisions at a centre-of-mass energy of 13 TeV and
correspond to an integrated luminosity of 3.2 fb−1. The
observed data are in agreement with the Standard Model
expectations. Exclusion limits are presented in models of
new phenomena including pair production of dark matter
candidates or large extra spatial dimensions. In a
simplified model of dark matter and an axial-vector
mediator, the search excludes mediator masses below 710 GeV
for dark matter candidate masses below 150 GeV. In an
effective theory of dark matter production, values of the
suppression scale M∗ up to 570 GeV are excluded and the
effect of truncation for various coupling values is
reported. For the ADD large extra spatial dimension model
the search places more stringent limits than earlier
searches in the same event topology, excluding MD up to
about 2.3 (2.8) TeV for two (six) additional spatial
dimensions; the limits are reduced by 20-40% depending on
the number of additional spatial dimensions when applying a
truncation procedure.},
Doi = {10.1007/JHEP06(2016)059},
Key = {fds321125}
}
@article{fds310327,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for new phenomena in events with a photon and missing
transverse momentum in pp collisions at √s =8 TeV with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.91.012008},
Abstract = {Results of a search for new phenomena in events with an
energetic photon and large missing transverse momentum with
the ATLAS experiment at the LHC are reported. Data were
collected in proton-proton collisions at a center-of-mass
energy of 8 TeV and correspond to an integrated luminosity
of 20.3 fb-1. The observed data are well described by the
expected Standard Model backgrounds. The expected (observed)
upper limit on the fiducial cross section for the production
of events with a photon and large missing transverse
momentum is 6.1 (5.3) fb at 95% confidence level. Exclusion
limits are presented on models of new phenomena with large
extra spatial dimensions, supersymmetric quarks, and direct
pair production of dark-matter candidates.},
Doi = {10.1103/PhysRevD.91.012008},
Key = {fds310327}
}
@article{fds315361,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP},
Title = {Search for new phenomena in events with at least three
photons collected in pp collisions at [Formula: see
text] = 8 TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {4},
Pages = {210},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4034-8},
Abstract = {Results of a search for new phenomena in events with at
least three photons are reported. Data from proton-proton
collisions at a centre-of-mass energy of 8 TeV,
corresponding to an integrated luminosity of 20.3
fb[Formula: see text], were collected with the ATLAS
detector at the LHC. The observed data are well described by
the Standard Model. Limits at the 95 % confidence level on
new phenomena are presented based on the rate of events in
an inclusive signal region and a restricted signal region
targeting the rare decay [Formula: see text], as well as
di-photon and tri-photon resonance searches. For a Standard
Model Higgs boson decaying to four photons via a pair of
intermediate pseudoscalar particles (<i>a</i>), limits are
found to be [Formula: see text] for 10 GeV [Formula: see
text] 62 GeV. Limits are also presented for Higgs boson-like
scalars (<i>H</i>) for [Formula: see text] 125 GeV, and for
a [Formula: see text] decaying to three photons via
[Formula: see text]. Additionally, the observed limit on the
branching ratio of the <i>Z</i> boson decay to three photons
is found to be BR[Formula: see text], a result five times
stronger than the previous result from LEP.},
Doi = {10.1140/epjc/s10052-016-4034-8},
Key = {fds315361}
}
@article{fds356634,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for new phenomena in events with same-charge leptons
and b-jets in pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {12},
Year = {2018},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2018)039},
Abstract = {A search for new phenomena in events with two same-charge
leptons or three leptons and jets identified as originating
from b-quarks in a data sample of 36.1 fb−1 of pp
collisions at s=13 TeV recorded by the ATLAS detector at the
Large Hadron Collider is reported. No significant excess is
found and limits are set on vector-like quark,
four-top-quark, and same-sign top-quark pair production. The
observed (expected) 95% CL mass limits for a vector-like T-
and B-quark singlet are mT > 0.98 (0.99) TeV and mB > 1.00
(1.01) TeV respectively. Limits on the production of the
vector-like T5/3-quark are also derived considering both
pair and single production; in the former case the lower
limit on the mass of the T5/3-quark is (expected to be) 1.19
(1.21) TeV. The Standard Model four-top-quark production
cross-section upper limit is (expected to be) 69 (29) fb.
Constraints are also set on exotic four-top-quark production
models. Finally, limits are set on same-sign top-quark pair
production. The upper limit on uu → tt production is
(expected to be) 89 (59) fb for a mediator mass of 1 TeV,
and a dark-matter interpretation is also derived, excluding
a mediator of 3 TeV with a dark-sector coupling of 1.0 and a
coupling to ordinary matter above 0.31.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP12(2018)039},
Key = {fds356634}
}
@article{fds307613,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for new phenomena in events with three charged
leptons at √s=7 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.87.052002},
Abstract = {A generic search for anomalous production of events with at
least three charged leptons is presented. The search uses a
pp-collision data sample at a center-of-mass energy of
√s=7 TeV corresponding to 4.6 fb-1 of integrated
luminosity collected in 2011 by the ATLAS detector at the
CERN Large Hadron Collider. Events are required to contain
at least two electrons or muons, while the third lepton may
either be an additional electron or muon, or a hadronically
decaying tau lepton. Events are categorized by the presence
or absence of a reconstructed tau-lepton or Z-boson
candidate decaying to leptons. No significant excess above
backgrounds expected from Standard Model processes is
observed. Results are presented as upper limits on event
yields from non-Standard-Model processes producing at least
three prompt, isolated leptons, given as functions of lower
bounds on several kinematic variables. Fiducial efficiencies
for model testing are also provided. The use of the results
is illustrated by setting upper limits on the production of
doubly charged Higgs bosons decaying to same-sign lepton
pairs.},
Doi = {10.1103/PhysRevD.87.052002},
Key = {fds307613}
}
@article{fds317298,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {Search for new phenomena in events with three or more
charged leptons in pp collisions at √s=8 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2015)138},
Abstract = {Abstract: A generic search for anomalous production of
events with at least three charged leptons is presented. The
data sample consists of pp collisions at √s=8 TeV
collected in 2012 by the ATLAS experiment at the CERN Large
Hadron Collider, and corresponds to an integrated luminosity
of 20.3 fb−1. Events are required to have at least three
selected lepton candidates, at least two of which must be
electrons or muons, while the third may be a hadronically
decaying tau. Selected events are categorized based on their
lepton flavour content and signal regions are constructed
using several kinematic variables of interest. No
significant deviations from Standard Model predictions are
observed. Model-independent upper limits on contributions
from beyond the Standard Model phenomena are provided for
each signal region, along with prescription to re-interpret
the limits for any model. Constraints are also placed on
models predicting doubly charged Higgs bosons and excited
leptons. For doubly charged Higgs bosons decaying to eτ or
μτ, lower limits on the mass are set at 400 GeV at 95%
confidence level. For excited leptons, constraints are
provided as functions of both the mass of the excited state
and the compositeness scale Λ, with the strongest mass
constraints arising in regions where the mass equals Λ. In
such scenarios, lower mass limits are set at 3.0 TeV for
excited electrons and muons, 2.5 TeV for excited taus, and
1.6 TeV for every excited-neutrino flavour.},
Doi = {10.1007/JHEP08(2015)138},
Key = {fds317298}
}
@article{fds356104,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for new phenomena in events with two opposite-charge
leptons, jets and missing transverse momentum in pp
collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {4},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2021)165},
Abstract = {The results of a search for direct pair production of top
squarks and for dark matter in events with two
opposite-charge leptons (electrons or muons), jets and
missing transverse momentum are reported, using 139 fb−1
of integrated luminosity from proton-proton collisions at s
= 13 TeV, collected by the ATLAS detector at the Large
Hadron Collider during Run 2 (2015–2018). This search
considers the pair production of top squarks and is
sensitive across a wide range of mass differences between
the top squark and the lightest neutralino. Additionally,
spin-0 mediator dark-matter models are considered, in which
the mediator is produced in association with a pair of top
quarks. The mediator subsequently decays to a pair of
dark-matter particles. No significant excess of events is
observed above the Standard Model background, and limits are
set at 95% confidence level. The results exclude top squark
masses up to about 1 TeV, and masses of the lightest
neutralino up to about 500 GeV. Limits on dark-matter
production are set for scalar (pseudoscalar) mediator masses
up to about 250 (300) GeV. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP04(2021)165},
Key = {fds356104}
}
@article{fds307809,
Author = {Kotwal, AV and Collaboration, CDF},
Title = {Search for new phenomena in events with two Z bosons and
missing transverse momentum in ppbar collisions at
sqrt(s)=1.96 TeV},
Journal = {Phys. Rev. D},
Volume = {85},
Number = {1},
Pages = {011104(R)},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.011104},
Abstract = {We present a search for new phenomena in events with two
reconstructed Z bosons and large missing transverse
momentum, sensitive to processes pp̄→X 2X 2→ZZX 1X 1,
where X 2 is an unstable particle decaying as X 2→ ZX 1
and X 1 is undetected. The particles X 1 and X 2 may be,
among other possibilities, fourth-generation neutrinos or
supersymmetric particles. We study the final state in which
one Z boson decays to two charged leptons and the second
decays hadronically. In data corresponding to an integrated
luminosity of 4.2fb -1 from proton-antiproton collisions
recorded by the CDF II detector at the Tevatron, with
center-of-mass energy of 1.96 TeV, we find agreement between
data and standard-model backgrounds. We calculate 95%
confidence level upper limits on the cross section of the
process pp̄→X 2X 2→ZZX 1X 1 ranging from 50 fb to 1 pb,
depending on the masses of X 1 and X 2. © 2012 American
Physical Society.},
Doi = {10.1103/PhysRevD.85.011104},
Key = {fds307809}
}
@article{fds310324,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
C},
Title = {Search for new phenomena in final states with an energetic
jet and large missing transverse momentum in pp
collisions at [Formula: see text]TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {299},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3517-3},
Abstract = {Results of a search for new phenomena in final states with
an energetic jet and large missing transverse momentum are
reported. The search uses 20.3 fb[Formula: see text] of
[Formula: see text] TeV data collected in 2012 with the
ATLAS detector at the LHC. Events are required to have at
least one jet with [Formula: see text] GeV and no leptons.
Nine signal regions are considered with increasing missing
transverse momentum requirements between [Formula: see
text] GeV and [Formula: see text] GeV. Good agreement is
observed between the number of events in data and Standard
Model expectations. The results are translated into
exclusion limits on models with either large extra spatial
dimensions, pair production of weakly interacting dark
matter candidates, or production of very light gravitinos in
a gauge-mediated supersymmetric model. In addition, limits
on the production of an invisibly decaying Higgs-like boson
leading to similar topologies in the final state are
presented.},
Doi = {10.1140/epjc/s10052-015-3517-3},
Key = {fds310324}
}
@article{fds321110,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for new phenomena in final states with an energetic
jet and large missing transverse momentum in pp collisions
at s =13 TeV using the ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032005},
Abstract = {Results of a search for new phenomena in final states with
an energetic jet and large missing transverse momentum are
reported. The search uses proton-proton collision data
corresponding to an integrated luminosity of 3.2 fb-1 at
s=13 TeV collected in 2015 with the ATLAS detector at the
Large Hadron Collider. Events are required to have at least
one jet with a transverse momentum above 250 GeV and no
leptons. Several signal regions are considered with
increasing missing-transverse-momentum requirements between
ETmiss>250 GeV and ETmiss>700 GeV. Good agreement is
observed between the number of events in data and Standard
Model predictions. The results are translated into exclusion
limits in models with large extra spatial dimensions, pair
production of weakly interacting dark-matter candidates, and
the production of supersymmetric particles in several
compressed scenarios.},
Doi = {10.1103/PhysRevD.94.032005},
Key = {fds321110}
}
@article{fds312133,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Search for new phenomena in final states with large jet
multiplicities and missing transverse momentum at √s = 8
TeV proton-proton collisions using the ATLAS
experiment},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {10},
Publisher = {Springer Nature},
Year = {2013},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2013)130},
Abstract = {A search is presented for new particles decaying to large
numbers (7 or more) of jets, with missing transverse
momentum and no isolated electrons or muons. This analysis
uses 20:3 fb-1 of pp collision data at √s = 8 TeV
collected by the ATLAS experiment at the Large Hadron
Collider. The sensitivity of the search is enhanced by
considering the number of b-tagged jets and the scalar sum
of masses of large-radius jets in an event. No evidence is
found for physics beyond the Standard Model. The results are
interpreted in the context of various simplified
supersymmetry-inspired models where gluinos are pair
produced, as well as an mSUGRA/CMSSM model. © SISSA
2013.},
Doi = {10.1007/JHEP10(2013)130},
Key = {fds312133}
}
@article{fds320777,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Search for new phenomena in final states with large jet
multiplicities and missing transverse momentum using √s =
7 TeV pp collisions with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2011},
Number = {11},
Publisher = {Springer Nature},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP11(2011)099},
Abstract = {Results are presented of a search for any particle(s)
decaying to six or more jets in association with missing
transverse momentum. The search is performed using
1.34fb−1 of √s = 7 TeV proton-proton collisions recorded
by the ATLAS detector during 2011. Data-driven techniques
are used to determine the backgrounds in kinematic regions
that require at least six, seven or eight jets, well beyond
the multiplicities required in previous analyses. No
evidence is found for physics beyond the Standard Model. The
results are interpreted in the context of a supersymmetry
model (MSUGRA/CMSSM) where they extend previous
constraints.},
Doi = {10.1007/JHEP11(2011)099},
Key = {fds320777}
}
@article{fds315359,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A},
Title = {Search for new phenomena in final states with large jet
multiplicities and missing transverse momentum with ATLAS
using √s=13 TeV proton–proton collisions},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {757},
Pages = {334-355},
Publisher = {Elsevier BV},
Year = {2016},
Month = {June},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2016.04.005},
Abstract = {Results are reported of a search for new phenomena, such as
supersymmetric particle production, that could be observed
in high-energy proton–proton collisions. Events with large
numbers of jets, together with missing transverse momentum
from unobserved particles, are selected. The data analysed
were recorded by the ATLAS experiment during 2015 using the
13 TeV centre-of-mass proton–proton collisions at the
Large Hadron Collider, and correspond to an integrated
luminosity of 3.2 fb−1. The search selected events with
various jet multiplicities from ≥7 to ≥10 jets, and with
various b-jet multiplicity requirements to enhance
sensitivity. No excess above Standard Model expectations is
observed. The results are interpreted within two
supersymmetry models, where gluino masses up to 1400 GeV are
excluded at 95% confidence level, significantly extending
previous limits.},
Doi = {10.1016/j.physletb.2016.04.005},
Key = {fds315359}
}
@article{fds359673,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armstrong, A and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Asquith, L and Assahsah, J and Assamagan, K and Astalos, R and Atkin,
RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Austrup, VA and Avolio, G and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Backman, F and Badea, A and Bagnaia, P and Bahrasemani, H and Bailey, AJ and Bailey,
VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Barron, U and Barsov, S and Bartels, F and Bartoldus, R and Bartolini, G and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Bauce, M and Bauer, F and Bauer, P and Bawa, HS and Bayirli, A and Beacham, JB and Beau,
T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov, VA and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
D and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
Kuutmann, E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer,
J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia
Bylund, O and Bethke, S and Betti, A and Bevan, AJ and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biesuz, NV and Biglietti,
M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Biswal, JP and Biswas, D and Bitadze, A and Bittrich, C and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr,
JTP and Burton, CD and Burzynski, JC and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo
Vazquez, CJ and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Caltabiano, A and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capua, M and Carbone, A and Cardarelli, R and Cardillo, F and Carducci, G and Carli,
T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carter, JWS and Carter, TM and Casadei, D and Casado,
MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia,
L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore,
JR and Cattai, A and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chau, CC and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, CL and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, YS and Christopher, LD and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Cioară, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM and Clark,
A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement, C and Clissa, L and Coadou, Y},
Title = {Search for New Phenomena in Final States with Two Leptons
and One or No b-Tagged Jets at sqrt[s]=13 TeV Using the
ATLAS Detector.},
Journal = {Physical review letters},
Volume = {127},
Number = {14},
Pages = {141801},
Year = {2021},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.127.141801},
Abstract = {A search for new phenomena is presented in final states with
two leptons and one or no b-tagged jets. The event selection
requires the two leptons to have opposite charge, the same
flavor (electrons or muons), and a large invariant mass. The
analysis is based on the full run-2 proton-proton collision
dataset recorded at a center-of-mass energy of
sqrt[s]=13 TeV by the ATLAS experiment at the LHC,
corresponding to an integrated luminosity of
139 fb^{-1}. No significant deviation from the expected
background is observed in the data. Inspired by the B-meson
decay anomalies, a four-fermion contact interaction between
two quarks (b, s) and two leptons (ee or μμ) is used as a
benchmark signal model, which is characterized by the energy
scale and coupling, Λ and g_{*}, respectively. Contact
interactions with Λ/g_{*} lower than 2.0 (2.4) TeV are
excluded for electrons (muons) at the 95% confidence level,
still far below the value that is favored by the B-meson
decay anomalies. Model-independent limits are set as a
function of the minimum dilepton invariant mass, which allow
the results to be reinterpreted in various signal
scenarios.},
Doi = {10.1103/physrevlett.127.141801},
Key = {fds359673}
}
@article{fds356712,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for new phenomena in high-mass diphoton final states
using 37 fb−1 of proton–proton collisions
collected at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {775},
Pages = {105-125},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2017.10.039},
Abstract = {Searches for new phenomena in high-mass diphoton final
states with the ATLAS experiment at the LHC are presented.
The analysis is based on pp collision data corresponding to
an integrated luminosity of 36.7 fb−1 at a centre-of-mass
energy s=13 TeV recorded in 2015 and 2016. Searches are
performed for resonances with spin 0, as predicted by
theories with an extended Higgs sector, and for resonances
with spin 2, using a warped extra-dimension model as a
benchmark model, as well as for non-resonant signals,
assuming a large extra-dimension scenario. No significant
deviation from the Standard Model is observed. Upper limits
are placed on the production cross section times branching
ratio to two photons as a function of the resonance mass. In
addition, lower limits are set on the ultraviolet cutoff
scale in the large extra-dimensions model.},
Doi = {10.1016/j.physletb.2017.10.039},
Key = {fds356712}
}
@article{fds347465,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Bakker, PJ and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot,
C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell,
AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair,
RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni,
A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cai, H and Cairo, VM and Cakir, O and Calace,
N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet,
S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini,
I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Search for new phenomena in high-mass final states with a
photon and a jet from pp collisions at s = 13 TeV with the
ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {2},
Pages = {102},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5553-2},
Abstract = {A search is performed for new phenomena in events having a
photon with high transverse momentum and a jet collected in
36.7 fb - 1 of proton-proton collisions at a centre-of-mass
energy of s = 13 TeV recorded with the ATLAS detector at
the Large Hadron Collider. The invariant mass distribution
of the leading photon and jet is examined to look for the
resonant production of new particles or the presence of new
high-mass states beyond the Standard Model. No significant
deviation from the background-only hypothesis is observed
and cross-section limits for generic Gaussian-shaped
resonances are extracted. Excited quarks hypothesized in
quark compositeness models and high-mass states predicted in
quantum black hole models with extra dimensions are also
examined in the analysis. The observed data exclude, at 95%
confidence level, the mass range below 5.3 TeV for excited
quarks and 7.1 TeV (4.4 TeV) for quantum black holes in
the Arkani-Hamed-Dimopoulos-Dvali (Randall-Sundrum) model
with six (one) extra dimensions.},
Doi = {10.1140/epjc/s10052-018-5553-2},
Key = {fds347465}
}
@article{fds307553,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Search for new phenomena in photon + jet events collected in
proton-proton collisions at √s = 8 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {728},
Number = {1},
Pages = {562-578},
Publisher = {Elsevier BV},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2013.12.029},
Abstract = {This Letter describes a model-independent search for the
production of new resonances in photon + jet (γ + jet)
events using 20 fb-1 of proton-proton LHC data recorded with
the ATLAS detector at a centre-of-mass energy of √s = 8
TeV. The γ + jet mass distribution is compared to a
background model fit from data; no significant deviation
from the background-only hypothesis is found. Limits are set
at 95% credibility level on generic Gaussian-shaped signals
and two benchmark phenomena beyond the Standard Model:
non-thermal quantum black holes and excited quarks.
Non-thermal quantum black holes are excluded below masses of
4.6 TeV and excited quarks are excluded below masses of 3.5
TeV. © 2013 The Authors. Published by Elsevier
B.V.},
Doi = {10.1016/j.physletb.2013.12.029},
Key = {fds307553}
}
@article{fds310296,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for new phenomena in the dijet mass distribution
using pp collision data at √s =8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.91.052007},
Abstract = {Dijet events produced in LHC proton-proton collisions at a
center-of-mass energy s=8 TeV are studied with the ATLAS
detector using the full 2012 data set, with an integrated
luminosity of 20.3 fb-1. Dijet masses up to about 4.5 TeV
are probed. No resonancelike features are observed in the
dijet mass spectrum. Limits on the cross section times
acceptance are set at the 95% credibility level for various
hypotheses of new phenomena in terms of mass or energy
scale, as appropriate. This analysis excludes excited quarks
with a mass below 4.06 TeV, color-octet scalars with a mass
below 2.70 TeV, heavy W′ bosons with a mass below 2.45
TeV, chiral W∗ bosons with a mass below 1.75 TeV, and
quantum black holes with six extra space-time dimensions
with threshold mass below 5.66 TeV.},
Doi = {10.1103/PhysRevD.91.052007},
Key = {fds310296}
}
@article{fds307636,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arika, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, R and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Urban, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Armadans,
RC and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella,
M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez,
VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas,
CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M},
Title = {Search for new phenomena in the WW → |v|′v′ final
state in pp collisions at √s=7 TeV with the ATLAS
detector},
Journal = {PHYSICS LETTERS B},
Volume = {718},
Number = {3},
Pages = {860-878},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2012.11.040},
Abstract = {This Letter reports a search for a heavy particle that
decays to WW using events produced in pp collisions at
s=7TeV. The data were recorded in 2011 by the ATLAS detector
and correspond to an integrated luminosity of 4.7 fb-1.
WW→ℓνℓ'ν'(ℓ, ℓ'=e or μ) final states are
considered and the distribution of the transverse mass of
the WW candidates is found to be consistent with Standard
Model expectations. Upper limits on the production cross
section times branching ratio into W boson pairs are set for
Randall-Sundrum and bulk Randall-Sundrum gravitons, which
result in observed 95% CL lower limits on the masses of the
two particles of 1.23 TeV and 0.84 TeV, respectively. ©
2012 CERN.},
Doi = {10.1016/j.physletb.2012.11.040},
Key = {fds307636}
}
@article{fds307715,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall,
J},
Title = {Search for new phenomena in tt events with large missing
transverse momentum in proton-proton collisions at sqrt[s] =
7 TeV with the ATLAS detector.},
Journal = {Physical review letters},
Volume = {108},
Number = {4},
Pages = {041805},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/physrevlett.108.041805},
Abstract = {A search for new phenomena in tt events with large missing
transverse momentum in proton-proton collisions at a
center-of-mass energy of 7 TeV is presented. The measurement
is based on 1.04 fb(-1) of data collected with the ATLAS
detector at the LHC. Contributions to this final state may
arise from a number of standard model extensions. The
results are interpreted in terms of a model where new
top-quark partners are pair produced and each decay to an
on-shell top (or antitop) quark and a long-lived undetected
neutral particle. The data are found to be consistent with
standard model expectations. A limit at 95% confidence level
is set excluding a cross section times branching ratio of
1.1 pb for a top-partner mass of 420 GeV and a neutral
particle mass less than 10 GeV. In a model of exotic fourth
generation quarks, top-partner masses are excluded up to 420
GeV and neutral particle masses up to 140
GeV.},
Doi = {10.1103/physrevlett.108.041805},
Key = {fds307715}
}
@article{fds376248,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Apyan, A and Aranzabal, N and Arcangeletti, C and Arce, ATH and Arena,
E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Arnaez, O and Arnold, H and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atashi, S and Atkin, RJ and Atkinson, M and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avolio, G and Axiotis,
K and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Baines, L and Bakalis, C and Baker, OK and Bakos, E and Bakshi Gupta and D and Balakrishnan, V and Balasubramanian,
R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barakat, M and Barberio,
EL and Barberis, D and Barbero, M and Barends, KN and Barillari, T and Barisits, M-S and Barklow, T and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barr, JD and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basan, A and Baselga, M and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia, M and Battulga, D and Bauce, M and Bauer, M and Bauer, P and Bazzano Hurrell and LT and Beacham, JB and Beau,
T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba,
L and Bellerive, A and Bellos, P and Beloborodov, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Bernardi, G and Bernius, C and Bernlochner, FU and Bernon, F and Berry,
T and Berta, P and Berthold, A and Bertram, IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Bianco, G and Biebel, O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Biros, M and Biryukov, S and Bisanz, T and Bisceglie, E and Biswal, JP and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Boehm, B and Bogavac,
D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold,
T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély,
AG and Bordulev, IS and Borecka-Bielska, HM and Borgna, LS and Borissov,
G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau, JE and Brener, R and Brenner, L and Brenner, R and Bressler, S and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Brown, LM and Bruce, LE and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Buanes, T and Buat, Q and Buchin, D and Buckley, AG and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burlayenko, O and Burr,
JTP and Burton, CD and Burzynski, JC and Busch, EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev, AR and Cabrera
Urbán, S and Cadamuro, L and Caforio, D and Cai, H and Cai, Y and Cairo,
VMM and Cakir, O and Calace, N and Calafiura, P and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson, BT and Carlson,
EM and Carminati, L and Carnelli, A and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
JWS and Carter, TM and Casado, MP and Caspar, M and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Cekmecelioglu, YC and Celebi, E and Celli, F and Centonze, MS and Cepaitis, V and Cerny, K and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cervato, B and Cervelli,
A and Cesarini, G and Cetin, SA and Chadi, Z and Chakraborty, D and Chan,
J and Chan, WY and Chapman, JD and Chapon, E and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chauhan, C and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, H and Chen, J and Chen, M and Chen, S and Chen, SJ and Chen, X and Chen,
Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chizhov, MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Chu, KL and Chu, MC and Chu, X and Chudoba,
J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio,
A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu, BM},
Title = {Search for New Phenomena in Two-Body Invariant Mass
Distributions Using Unsupervised Machine Learning for
Anomaly Detection at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {132},
Number = {8},
Pages = {081801},
Year = {2024},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.132.081801},
Abstract = {Searches for new resonances are performed using an
unsupervised anomaly-detection technique. Events with at
least one electron or muon are selected from
140 fb^{-1} of pp collisions at sqrt[s]=13 TeV
recorded by ATLAS at the Large Hadron Collider. The approach
involves training an autoencoder on data, and subsequently
defining anomalous regions based on the reconstruction loss
of the decoder. Studies focus on nine invariant mass spectra
that contain pairs of objects consisting of one light jet or
b jet and either one lepton (e,μ), photon, or second light
jet or b jet in the anomalous regions. No significant
deviations from the background hypotheses are observed.
Limits on contributions from generic Gaussian signals with
various widths of the resonance mass are obtained for nine
invariant masses in the anomalous regions.},
Doi = {10.1103/physrevlett.132.081801},
Key = {fds376248}
}
@article{fds347478,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and AlconadaVerzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and AlvarezGonzalez,
B and ÁlvarezPiqueras, D and Alviggi, MG and Amadio, BT and AmaralCoutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor
DosSantos, SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and AraujoFerraz, V and Pereira, RA and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Baker, OK and Bakker, PJ and Gupta, DB and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee,
S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli,
A and Barone, G and Barr, AJ and BarrancoNavarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and BenharNoccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and BessidskaiaBylund, O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini,
C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black,
JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner,
D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona,
M and Bonilla, JSB and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and BossioSola, JD and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt,
A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin,
DL and Bristow, TM and Britton, D and Britzger, D and Brock, I and Brock,
R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman deRenstrom, PA and Bruncko, D and Bruni,
A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard,
CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and CabreraUrbán, S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and CalventeLopez, S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and CamachoToro, R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and CanoBret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and CastilloGimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and CerdaAlberich, L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
DC and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui ElMoursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
IA and Ciocio, A and Cirotto, F and Citron, ZH},
Title = {Search for new phenomena using the invariant mass
distribution of same-flavour opposite-sign dilepton pairs in
events with missing transverse momentum in s=13
Tepp collisions with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {8},
Pages = {625},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-6081-9},
Abstract = {A search for new phenomena in final states containing an
e+e- or μ+μ- pair, jets, and large missing transverse
momentum is presented. This analysis makes use of
proton-proton collision data with an integrated luminosity
of 36.1fb-1 , collected during 2015 and 2016 at a
centre-of-mass energy s=13TeV with the ATLAS detector at the
Large Hadron Collider. The search targets the pair
production of supersymmetric coloured particles (squarks or
gluinos) and their decays into final states containing an
e+e- or μ+μ- pair and the lightest neutralino ( χ~10 )
via one of two next-to-lightest neutralino ( χ~20 ) decay
mechanisms: χ~20→Zχ~10 , where the <i>Z</i> boson decays
leptonically leading to a peak in the dilepton invariant
mass distribution around the <i>Z</i> boson mass; and
χ~20→ℓ+ℓ-χ~10 with no intermediate ℓ+ℓ-
resonance, yielding a kinematic endpoint in the dilepton
invariant mass spectrum. The data are found to be consistent
with the Standard Model expectation. Results are interpreted
using simplified models, and exclude gluinos and squarks
with masses as large as 1.85 and 1.3 Te at 95% confidence
level, respectively.},
Doi = {10.1140/epjc/s10052-018-6081-9},
Key = {fds347478}
}
@article{fds356715,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for new phenomena with large jet multiplicities and
missing transverse momentum using large-radius jets and
flavour-tagging at ATLAS in 13 TeV pp collisions},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {12},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2017)034},
Abstract = {A search is presented for particles that decay producing a
large jet multiplicity and invisible particles. The event
selection applies a veto on the presence of isolated
electrons or muons and additional requirements on the number
of b-tagged jets and the scalar sum of masses of
large-radius jets. Having explored the full ATLAS 2015-2016
dataset of LHC proton-proton collisions at s=13 TeV, which
corresponds to 36.1 fb−1 of integrated luminosity, no
evidence is found for physics beyond the Standard Model. The
results are interpreted in the context of simplified models
inspired by R-parity-conserving and R-parity-violating
supersymmetry, where gluinos are pair-produced. More generic
models within the phenomenological minimal supersymmetric
Standard Model are also considered.},
Doi = {10.1007/JHEP12(2017)034},
Key = {fds356715}
}
@article{fds356776,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Search for new phenomena with photon+jet events in
proton-proton collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {3},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2016)041},
Abstract = {Abstract: A search is performed for the production of
high-mass resonances decaying into a photon and a jet in 3.2
fb−1of proton-proton collisions at a centre-of-mass energy
of (Formula presented.) TeV collected by the ATLAS detector
at the Large Hadron Collider. Selected events have an
isolated photon and a jet, each with transverse momentum
above 150 GeV. No significant deviation of the γ+jet
invariant mass distribution from the background-only
hypothesis is found. Limits are set at 95% confidence level
on the cross sections of generic Gaussian-shaped signals and
of a few benchmark phenomena beyond the Standard Model:
excited quarks with vector-like couplings to the Standard
Model particles, and non-thermal quantum black holes in two
models of extra spatial dimensions. The minimum excluded
visible cross sections for Gaussian-shaped resonances with
width-to-mass ratios of 2% decrease from about 6 fb for a
mass of 1.5 TeV to about 0.8 fb for a mass of 5 TeV. The
minimum excluded visible cross sections for Gaussian-shaped
resonances with width-to-mass ratios of 15% decrease from
about 50 fb for a mass of 1.5 TeV to about 1.0 fb for a mass
of 5 TeV. Excited quarks are excluded below masses of 4.4
TeV, and non-thermal quantum black holes are excluded below
masses of 3.8 (6.2) TeV for Randall-Sundrum
(Arkani-Hamed-Dimopoulous-Dvali) models with one (six) extra
dimensions.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP03(2016)041},
Key = {fds356776}
}
@article{fds307863,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R},
Title = {Search for new phenomena with the monojet and missing
transverse momentum signature using the ATLAS detector in
s=7TeV proton-proton collisions},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {705},
Number = {4},
Pages = {294-312},
Publisher = {Elsevier BV},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2011.10.006},
Abstract = {A search for new phenomena in events featuring a high energy
jet and large missing transverse momentum in proton-proton
collisions at s=7TeV is presented using a dataset
corresponding to an integrated luminosity of 33 pb-1
recorded with the ATLAS detector at the Large Hadron
Collider. The number of observed events is consistent with
the Standard Model prediction. This result is interpreted in
terms of limits on a model of Large Extra Dimensions. ©
2011 CERN.},
Doi = {10.1016/j.physletb.2011.10.006},
Key = {fds307863}
}
@article{fds356105,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for new phenomena with top quark pairs in final
states with one lepton, jets, and missing transverse
momentum in pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2021)174},
Abstract = {A search for new phenomena with top quark pairs in final
states with one isolated electron or muon, multiple jets,
and large missing transverse momentum is performed. Signal
regions are designed to search for two-, three-, and
four-body decays of the directly pair-produced
supersymmetric partner of the top quark (stop). Additional
signal regions are designed specifically to search for
spin-0 mediators that are produced in association with a
pair of top quarks and decay into a pair of dark-matter
particles. The search is performed using the Large Hadron
Collider proton-proton collision dataset at a centre-of-mass
energy of s = 13 TeV recorded by the ATLAS detector from
2015 to 2018, corresponding to an integrated luminosity of
139 fb−1. No significant excess above the Standard Model
background is observed, and limits at 95% confidence level
are set in the stop-neutralino mass plane and as a function
of the mediator mass or the dark-matter particle mass. Stops
are excluded up to 1200 GeV (710 GeV) in the two-body
(three-body) decay scenario. In the four-body scenario stops
up to 640 GeV are excluded for a stop-neutralino mass
difference of 60 GeV. Scalar and pseudoscalar dark-matter
mediators are excluded up to 200 GeV when the coupling
strengths of the mediator to Standard Model and dark-matter
particles are both equal to one and when the mass of the
dark-matter particle is 1 GeV. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP04(2021)174},
Key = {fds356105}
}
@article{fds307835,
Author = {Aaltonen, TEA},
Title = {Search for New Physics in High ${p}_{T}$ Like-Sign Dilepton
Events at {CDF II}},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {18},
Pages = {181801},
Publisher = {American Physical Society},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.181801},
Abstract = {We present a search for new physics in events with two high
pT leptons of the same electric charge, using data with an
integrated luminosity of 6.1 fb(-1). The observed data are
consistent with standard model predictions. We set 95% C.L.
lower limits on the mass of doubly charged scalars decaying
to like-sign dileptons, m(H±±) > 190-245 GeV/c(2),
assuming 100% BR to ee, μμ or eμ.},
Doi = {10.1103/PhysRevLett.107.181801},
Key = {fds307835}
}
@article{fds308050,
Author = {Aaltonen, and T, and others},
Title = {Search for new physics in high mass electron-positron events
in $p \bar{p}$ collisions at $\sqrt{s}$ =
1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {99},
Number = {17},
Pages = {171802},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.99.171802},
Abstract = {We report the results of a search for a narrow resonance in
electron-positron events in the invariant mass range of
150--950 GeV/c2 using 1.3 fb-1 of p[overline p] collision
data at sqrt(s)=1.96 TeV collected by the CDF II detector at
Fermilab. No significant evidence of such a resonance is
observed and we interpret the results to exclude the
standard-model-like Z[prime] with a mass below 923 GeV/c2
and the Randall-Sundrum graviton with a mass below 807
GeV/c2 for k/[overline M]pl=0.1, both at the 95\% confidence
level. Combining with diphoton data excludes the
Randall-Sundrum graviton for masses below 889 GeV/c2 for
k/[overline M]pl=0.1.},
Doi = {10.1103/physrevlett.99.171802},
Key = {fds308050}
}
@article{fds308091,
Author = {Abulencia, and A, and others},
Title = {Search for new physics in lepton + photon + X events with
305-pb**(-1) of p anti-p collisions at s**(1/2) = 1.96-
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {97},
Number = {3},
Pages = {031801},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.97.031801},
Abstract = {We present results of a search for anomalous production of
events containing a charged lepton (either electron or muon)
and a photon, both with high transverse momentum,
accompanied by additional signatures, X, including missing
transverse energy (MET) and additional leptons and photons.
We use the same kinematic selection criteria as in a
previous CDF search, but with a substantially larger data
set, 305 pb-1, a ppbar collision energy of 1.96 TeV, and the
upgraded CDF II detector. We find 42 Lepton+Photon+MET
events versus a standard model expectation of 37.3 +- 5.4
events. The level of excess observed in Run I, 16 events
with an expectation of 7.6 +- 0.7 events (corresponding to a
2.7 sigma effect), is not supported by the new data. In the
signature of Multi-Lepton+Photon+X we observe 31 events
versus an expectation of 23.0 +- 2.7 events. In this sample
we find no events with an extra photon or MET and so find no
events like the one ee+gg+MET event observed in Run
I.},
Doi = {10.1103/physrevlett.97.031801},
Key = {fds308091}
}
@article{fds307754,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Search for new physics in the dijet mass distribution using
1 fb -1 of pp collision data at √s=7 TeV
collected by the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {708},
Number = {1-2},
Pages = {37-54},
Publisher = {Elsevier BV},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2012.01.035},
Abstract = {Invariant mass distributions of jet pairs (dijets) produced
in LHC proton-proton collisions at a centre-of-mass energy
s=7 TeV have been studied using a data set corresponding to
an integrated luminosity of 1.0 fb -1 recorded in 2011 by
ATLAS. Dijet masses up to ~4 TeV are observed in the data,
and no evidence of resonance production over background is
found. Limits are set at 95% C.L. for several new physics
hypotheses: excited quarks are excluded for masses below 299
TeV, axigluons are excluded for masses below 3.32 TeV, and
colour octet scalar resonances are excluded for masses below
1.92 TeV. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.01.035},
Key = {fds307754}
}
@article{fds307972,
Author = {Aaltonen, T and others},
Title = {Search for new physics in the mu mu + e/mu + E-slash [sub T]
channel with a low-p[sub T] lepton threshold at the Collider
Detector at Fermilab},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {5},
Pages = {052004},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.052004},
Abstract = {A search for new physics using three-lepton (trilepton) data
collected with the CDF II detector and corresponding to an
integrated luminosity of 976 pb-1 is presented. The standard
model predicts a low rate of trilepton events, which makes
some supersymmetric processes, such as chargino-neutralino
production, measurable in this channel. The μμ+ signature
is investigated, where ℓ is an electron or a muon, with
the additional requirement of large missing transverse
energy. In this analysis, the lepton transverse momenta with
respect to the beam direction (pT) are as low as 5GeV/c, a
selection that improves the sensitivity to particles that
are light as well as to ones that result in leptonically
decaying tau leptons. At the same time, this low-pT
selection presents additional challenges due to the
non-negligible heavy-quark background at low lepton momenta.
This background is measured with an innovative technique
using experimental data. Several dimuon and trilepton
control regions are investigated, and good agreement between
experimental results and standard-model predictions is
observed. In the signal region, we observe one three-muon
event and expect 0.4±0.1μμ+ events from standard-model
processes. © 2009 The American Physical
Society.},
Doi = {10.1103/PhysRevD.79.052004},
Key = {fds307972}
}
@article{fds312131,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Search for new physics in trilepton events and limits on the
associated chargino-neutralino production at
CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {1},
Pages = {012011},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.90.012011},
Abstract = {We perform a search for new physics using final states
consisting of three leptons and a large imbalance in
transverse momentum resulting from proton-antiproton
collisions at 1.96 TeV center-of-mass energy. We use data
corresponding to 5.8fb-1 of integrated luminosity recorded
by the CDF II detector at the Tevatron collider. Our main
objective is to investigate possible new low-momentum (down
to 5GeV/c) multileptonic final states not investigated by
LHC experiments. Relative to previous CDF analyses, we
expand the geometric and kinematic coverage of electrons and
muons and utilize tau leptons that decay hadronically.
Inclusion of tau leptons is particularly important for
supersymmetry (SUSY) searches. The results are consistent
with standard-model predictions within 1.85σ. By optimizing
our event selection to increase sensitivity to the minimal
supergravity (mSUGRA) SUSY model, we set limits on the
associated production of chargino and next-to-lightest
neutralino, the SUSY partners of the electroweak gauge
bosons. We exclude cross sections up to 0.1 pb and chargino
masses up to 168GeV/c2 at 95% C.L., for a suitable set of
mSUGRA parameters. We also exclude a region of the
two-dimensional space of the masses of the neutralino and
the supersymmetric partner of the tau lepton, not previously
excluded at the Tevatron. © 2014 American Physical
Society.},
Doi = {10.1103/PhysRevD.90.012011},
Key = {fds312131}
}
@article{fds308209,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee,
S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz,
D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cummings, MAC and Cutts,
D and Dahl, OI and Davis, GA and Davis, K and De, K and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov,
VN},
Title = {Search for new physics in [formula presented] data at DØ
using SLEUTH: A quasi-model-independent search strategy for
new physics},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {62},
Number = {9},
Pages = {19},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.62.092004},
Abstract = {We present a quasi-model-independent search for the physics
responsible for electroweak symmetry breaking. We define
final states to be studied, and construct a rule that
identifies a set of relevant variables for any particular
final state. A new algorithm (“SLEUTH”) searches for
regions of excess in those variables and quantifies the
significance of any detected excess. After demonstrating the
sensitivity of the method, we apply it to the semi-inclusive
channel (Formula presented) collected in 108 (Formula
presented) of (Formula presented) collisions at (Formula
presented) TeV at the DØ experiment during 1992–1996 at
the Fermilab Tevatron. We find no evidence of new high
(Formula presented) physics in this sample. © 2000 The
American Physical Society.},
Doi = {10.1103/PhysRevD.62.092004},
Key = {fds308209}
}
@article{fds308187,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MA and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Duperrin, A and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher,
S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Fox, H and Frame, KC and Fu,
S and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin,
R and Ginther, G and Gómez, B and Gómez, G and Goncharov, PI and González Solís and JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Grinstein, S and Groer, L and Grünendahl, S and Gupta,
A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Heuring, T and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Huang, Y and Illingworth, R and Ito, AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jones, M and Jöstlein, H and Juste, A and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Ke, Z and Kehoe, R and Khanov, A and Kharchilava, A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kothari, B and Kotwal,
AV and Kozelov, AV and Kozlovsky, EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Lee, WM and Leflat, A and Leggett, C and Lehner, F and Li, J and Li, QZ and Li, X and Lima, JG and Lincoln, D and Linn, SL and Linnemann, J and Lipton,
R and Lucotte, A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AK and Madaras, RJ and Malyshev, VL and Manankov, V and Mao, HS and Marshall,
T and Martin, MI and Martin, RD and Mauritz, KM and May, B and Mayorov, AA and McCarthy, R and McMahon, T and Melanson, HL and Merkin, M and Merritt,
KW and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov,
N and Mondal, NK and Montgomery, HE and Moore, RW and Mostafa, M and da
Motta, H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Neal,
HA and Negret, JP and Negroni, S and Nunnemann, T and O'Neil, D and Oguri,
V and Olivier, B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou,
K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, M and Peters, O and Pétroff, P and Piegaia, R and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Qian, J and Raja, R and Rajagopalan, S and Ramberg,
E and Rapidis, PA and Reay, NW and Reucroft, S and Ridel, M and Rijssenbeek, M and Rizatdinova, F and Rockwell, T and Roco, M and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Sajot,
G and Santoro, A and Sawyer, L and Schamberger, RD and Schellman, H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov,
D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton,
NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stone, A and Stoyanova, DA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and van Gemmeren, P and Vaniev, V and Van Kooten and R and Varelas, N and Vertogradov, LS and Villeneuve-Seguier, F and Volkov,
AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, ZM and Warchol, J and Watts, G and Wayne, M and Weerts, H and White, A and White, JT and Whiteson, D and Wightman, JA and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zheng, H and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev, EG and Zylberstejn,
A},
Title = {Search for new physics using QUAERO: a general interface to
D0 event data.},
Journal = {Physical review letters},
Volume = {87},
Number = {23},
Pages = {231801},
Year = {2001},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.87.231801},
Abstract = {We describe QUAERO, a method that (i) enables the automatic
optimization of searches for physics beyond the standard
model, and (ii) provides a mechanism for making high energy
collider data generally available. We apply QUAERO to
searches for standard model WW, ZZ, and t t macro
production, to searches for these objects produced through a
new heavy resonance, and to the first direct search for
W'-->WZ. Through this interface, we make three data sets
collected by the D0 experiment at square root of [s] = 1.8
TeV publicly available.},
Doi = {10.1103/physrevlett.87.231801},
Key = {fds308187}
}
@article{fds307897,
Author = {Aaltonen, and T, and others},
Title = {Search for New Physics with a Dijet Plus Missing $E_{T}$
Signature in $pp[over \ifmmode\bar\else\textasciimacron\fi{}]$
Collisions at $\sqrt{s}=1.96\,\,TeV$},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {13},
Pages = {131801},
Publisher = {American Physical Society},
Year = {2010},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.131801},
Abstract = {We present results of a signature-based search for new
physics using a dijet plus missing transverse energy (E(T))
data sample collected in 2 fb⁻¹ of pp collisions at
√s=1.96 TeV with the CDF II detector at the Fermilab
Tevatron. We observe no significant event excess with
respect to the standard model prediction and extract a 95%
C.L. upper limit on the cross section times acceptance for a
potential contribution from a nonstandard model process. The
search is made by using novel, data-driven techniques for
estimating backgrounds that are applicable to first searches
at the LHC.},
Doi = {10.1103/PhysRevLett.105.131801},
Key = {fds307897}
}
@article{fds356760,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for new resonances decaying to a W or Z boson and a
Higgs boson in the ℓ+ℓ−bb¯,
ℓνbb¯, and νν¯bb¯ channels with pp collisions at
s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {765},
Pages = {32-52},
Year = {2017},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2016.11.045},
Abstract = {A search is presented for new resonances decaying to a W or
Z boson and a Higgs boson in the ℓ+ℓ−bb¯, ℓνbb¯,
and νν¯bb¯ channels in pp collisions at s=13 TeV with
the ATLAS detector at the Large Hadron Collider using a
total integrated luminosity of 3.2 fb−1. The search is
conducted by looking for a localized excess in the WH/ZH
invariant or transverse mass distribution. No significant
excess is observed, and the results are interpreted in terms
of constraints on a simplified model based on a
phenomenological Lagrangian of heavy vector
triplets.},
Doi = {10.1016/j.physletb.2016.11.045},
Key = {fds356760}
}
@article{fds321074,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for new resonances in events with one lepton and
missing transverse momentum in pp collisions at √s=13 TeV
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {762},
Pages = {334-352},
Publisher = {Elsevier BV},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2016.09.040},
Abstract = {A search for W′ bosons in events with one lepton (electron
or muon) and missing transverse momentum is presented. The
search uses 3.2 fb−1 of pp collision data collected at
s=13 TeV by the ATLAS experiment at the LHC in 2015. The
transverse mass distribution is examined and no significant
excess of events above the level expected from Standard
Model processes is observed. Upper limits on the W′ boson
cross-section times branching ratio to leptons are set as a
function of the W′ mass. Within the Sequential Standard
Model W′ masses below 4.07 TeV are excluded at the 95%
confidence level. This extends the limit set using LHC data
at s=8 TeV by around 800 GeV.},
Doi = {10.1016/j.physletb.2016.09.040},
Key = {fds321074}
}
@article{fds349431,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Search for new resonances in mass distributions of jet pairs
using 139 fb −1 of pp collisions at √s = 13
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {3},
Year = {2020},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2020)145},
Abstract = {A search for new resonances decaying into a pair of jets is
reported using the dataset of proton-proton collisions
recorded at s = 13 TeV with the ATLAS detector at the Large
Hadron Collider between 2015 and 2018, corresponding to an
integrated luminosity of 139 fb−1. The distribution of the
invariant mass of the two leading jets is examined for local
excesses above a data-derived estimate of the Standard Model
background. In addition to an inclusive dijet search, events
with jets identified as containing b-hadrons are examined
specifically. No significant excess of events above the
smoothly falling background spectra is observed. The results
are used to set cross-section upper limits at 95% confidence
level on a range of new physics scenarios. Model-independent
limits on Gaussian-shaped signals are also reported. The
analysis looking at jets containing b-hadrons benefits from
improvements in the jet flavour identification at high
transverse momentum, which increases its sensitivity
relative to the previous analysis beyond that expected from
the higher integrated luminosity. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP03(2020)145},
Key = {fds349431}
}
@article{fds310344,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for new resonances in Wγ and Zγ final states in pp
collisions at √s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {738},
Pages = {428-447},
Publisher = {Elsevier BV},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2014.10.002},
Abstract = {This letter presents a search for new resonances decaying to
final states with a vector boson produced in association
with a high transverse momentum photon, Vγ with
V=W(→ℓν) or Z(→ℓ+ℓ−), where ℓ=e or μ. The
measurements use 20.3 fb−1 of proton–proton collision
data at a center–of–mass energy of s=8 TeV recorded with
the ATLAS detector. No deviations from the Standard Model
expectations are found, and production cross section limits
are set at 95% confidence level. Masses of the hypothetical
aT and ωT states of a benchmark Low Scale Technicolor model
are excluded in the ranges [275,960] GeV and
[200,700]∪[750,890] GeV, respectively. Limits at 95%
confidence level on the production cross section of a
singlet scalar resonance decaying to Zγ final states have
also been obtained for masses below 1180
GeV.},
Doi = {10.1016/j.physletb.2014.10.002},
Key = {fds310344}
}
@article{fds356540,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Search for non-resonant Higgs boson pair production in the
bbℓνℓν final state with the ATLAS detector in pp
collisions at s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {801},
Year = {2020},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2019.135145},
Abstract = {A search for non-resonant Higgs boson pair production, as
predicted by the Standard Model, is presented, where one of
the Higgs bosons decays via the H→bb channel and the other
via one of the H→WW⁎/ZZ⁎/ττ channels. The analysis
selection requires events to have at least two b-tagged jets
and exactly two leptons (electrons or muons) with opposite
electric charge in the final state. Candidate events
consistent with Higgs boson pair production are selected
using a multi-class neural network discriminant. The
analysis uses 139 fb−1 of pp collision data recorded at a
centre-of-mass energy of 13 TeV by the ATLAS detector at the
Large Hadron Collider. An observed (expected) upper limit of
1.2 (0.9−0.3+0.4) pb is set on the non-resonant Higgs
boson pair production cross-section at 95% confidence level,
which is equivalent to 40 (29−9+14) times the value
predicted in the Standard Model.},
Doi = {10.1016/j.physletb.2019.135145},
Key = {fds356540}
}
@article{fds375848,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes
Flores, CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani,
C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso,
M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos,
SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Search for non-resonant production of semi-visible jets
using Run 2 data in ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {848},
Pages = {138324-138324},
Publisher = {Elsevier BV},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138324},
Abstract = {Semi-visible jets, with a significant contribution to the
event's missing transverse momentum, can arise in strongly
interacting dark sectors. This results in an event topology
where one of the jets can be aligned with the direction of
the missing transverse momentum. The first search for
semi-visible jets produced via a t-channel mediator exchange
is presented. The analysis uses proton-proton collisions
with an integrated luminosity of 139 fb−1 and a
centre-of-mass energy of 13 TeV, collected with the ATLAS
detector during the Run 2 of the LHC. No excess over
Standard Model predictions is observed. Assuming a coupling
strength of unity between the mediator, a Standard Model
quark and a dark quark, mediator masses up to 2.7 TeV are
excluded at the 95% confidence level. Upper limits on the
coupling strength are also derived.},
Doi = {10.1016/j.physletb.2023.138324},
Key = {fds375848}
}
@article{fds310338,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F},
Title = {Search for nonpointing and delayed photons in the diphoton
and missing transverse momentum final state in 8 TeV pp
collisions at the LHC using the ATLAS detector SEARCH for
NONPOINTING and DELAYED PHOTONS in ⋯ G. AAD et
al.},
Journal = {Zeitschrift fur Antikes Christentum},
Volume = {19},
Number = {3},
Pages = {1DUMMY},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.90.112005},
Abstract = {© 2014 CERN. © 2014 CERN, for the ATLAS Collaboration.
Published by the American Physical Society under the terms
of the »http://creativecommons.org/licenses/by/3.0/»
Creative Commons Attribution 3.0 License. Further
distribution of this work must maintain attribution to the
author(s) and the published article's title, journal
citation, and DOI.A search has been performed, using the
full 20.3 fb-1 data sample of 8 TeV proton-proton collisions
collected in 2012 with the ATLAS detector at the LHC, for
photons originating from a displaced vertex due to the decay
of a neutral long-lived particle into a photon and an
invisible particle. The analysis investigates the diphoton
plus missing transverse momentum final state, and is
therefore most sensitive to pair production of long-lived
particles. The analysis technique exploits the capabilities
of the ATLAS electromagnetic calorimeter to make precise
measurements of the flight direction, as well as the time of
flight, of photons. No excess is observed over the Standard
Model predictions for background. Exclusion limits are set
within the context of gauge mediated supersymmetry breaking
models, with the lightest neutralino being the
next-to-lightest supersymmetric particle and decaying into a
photon and gravitino with a lifetime in the range from 250
ps to about 100 ns.},
Doi = {10.1103/PhysRevD.90.112005},
Key = {fds310338}
}
@article{fds307591,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Search for nonpointing photons in the diphoton and ETmiss
final state in √s=7 TeV proton-proton collisions using the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.88.012001},
Abstract = {A search has been performed for photons originating in the
decay of a neutral long-lived particle, exploiting the
capabilities of the ATLAS electromagnetic calorimeter to
make precise measurements of the flight direction of
photons, as well as the calorimeter's excellent time
resolution. The search has been made in the diphoton plus
missing transverse energy final state, using the full data
sample of 4.8 fb-1 of 7 TeV proton-proton collisions
collected in 2011 with the ATLAS detector at the LHC. No
excess is observed above the background expected from
Standard Model processes. The results are used to set
exclusion limits in the context of gauge mediated
supersymmetry breaking models, with the lightest neutralino
being the next-to-lightest supersymmetric particle and
decaying with a lifetime in excess of 0.25 ns into a photon
and a gravitino. © 2013 CERN.},
Doi = {10.1103/PhysRevD.88.012001},
Key = {fds307591}
}
@article{fds373909,
Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Arnaez, O and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin, T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi, G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori, G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
Title = {Search for nonresonant pair production of Higgs bosons in
the bb¯bb¯ final state in pp collisions at √s = 13 TeV
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {108},
Number = {5},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.108.052003},
Abstract = {A search for nonresonant Higgs boson pair production in the
Formula Presented final state is presented. The analysis
uses Formula Presented of Formula Presented collision data
at Formula Presented collected with the ATLAS detector at
the Large Hadron Collider, and targets both the gluon-gluon
fusion and vector-boson fusion production modes. No evidence
of the signal is found and the observed (expected) upper
limit on the cross section for nonresonant Higgs boson pair
production is determined to be 5.4 (8.1) times the Standard
Model predicted cross section at 95% confidence level.
Constraints are placed on modifiers to the Formula Presented
and Formula Presented couplings. The observed (expected)
Formula Presented constraints on the Formula Presented
coupling modifier, Formula Presented, are determined to be
Formula Presented (Formula Presented), while the
corresponding constraints for the Formula Presented coupling
modifier, Formula Presented, are Formula Presented (Formula
Presented). In addition, constraints on relevant
coefficients are derived in the context of the Standard
Model effective field theory and Higgs effective field
theory, and upper limits on the Formula Presented production
cross section are placed in seven Higgs effective field
theory benchmark scenarios.},
Doi = {10.1103/PhysRevD.108.052003},
Key = {fds373909}
}
@article{fds356791,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Search for nonstandard higgs bosons using high mass photon
pairs in p¯p→γγ+2 jets at √s=1.8TeV},
Journal = {Physical Review Letters},
Volume = {82},
Number = {11},
Pages = {2244-2249},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.2244},
Abstract = {A search has been carried out for events in the channel
p¯p→γγ+2 Such a signature can characterize the
production of a nonstandard Higgs boson together with a W or
Z boson. We refer to this nonstandard Higgs, having standard
model couplings to vector bosons but no coupling to
fermions, as a “bosonic Higgs.” With the requirement of
two high transverse energy photons and two jets, the
diphoton mass (mγγ) distribution is consistent with
expected background. A 90 (95)% confidence level (C.L.)
upper limit on the cross section as a function of mass is
calculated, ranging from 0.60 (0.80) pb for mγγ =65GeV/c2
to 0.26 (0.34) pb for mγγ=150GeV/c2, corresponding to a
95% C.L. lower limit on the mass of a bosonic Higgs of
78.5GeV/c2. © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.82.2244},
Key = {fds356791}
}
@article{fds310345,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for pair and single production of new heavy quarks
that decay to a Z boson and a third-generation quark in pp
collisions at √ S = 8TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {11},
Publisher = {Springer Nature},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2014)104},
Abstract = {Abstract: A search is presented for the production of new
heavy quarks that decay to a Z boson and a third-generation
Standard Model quark. In the case of a new charge +2/3 quark
(T ), the decay targeted is T → Zt, while the decay
targeted for a new charge −1/3 quark (B) is B → Zb. The
search is performed with a dataset corresponding to 20.3
fb−1 of pp collisions at (Formula presented.) TeV recorded
in 2012 with the ATLAS detector at the CERN Large Hadron
Collider. Selected events contain a high transverse momentum
Z boson candidate reconstructed from a pair of oppositely
charged same-flavor leptons (electrons or muons), and are
analyzed in two channels defined by the absence or presence
of a third lepton. Hadronic jets, in particular those with
properties consistent with the decay of a b-hadron, are also
required to be present in selected events. Different
requirements are made on the jet activity in the event in
order to enhance the sensitivity to either heavy quark pair
production mediated by the strong interaction, or single
production mediated by the electroweak interaction. No
significant excess of events above the Standard Model
expectation is observed, and lower limits are derived on the
mass of vector-like T and B quarks under various branching
ratio hypotheses, as well as upper limits on the magnitude
of electroweak coupling parameters.},
Doi = {10.1007/JHEP11(2014)104},
Key = {fds310345}
}
@article{fds356636,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for pair and single production of vectorlike quarks
in final states with at least one Z boson decaying into a
pair of electrons or muons in pp collision data collected
with the ATLAS detector at s =13 TeV},
Journal = {Physical Review D},
Volume = {98},
Number = {11},
Year = {2018},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.98.112010},
Abstract = {A search for vectorlike quarks is presented, which targets
their decay into a Z boson and a third-generation Standard
Model quark. In the case of a vectorlike quark T (B) with
charge +2/3e (-1/3e), the decay searched for is T→Zt
(B→Zb). Data for this analysis were taken during 2015 and
2016 with the ATLAS detector at the Large Hadron Collider
and correspond to an integrated luminosity of 36.1 fb-1 of
pp collisions at s=13 TeV. The final state used is
characterized by the presence of b-tagged jets, as well as a
Z boson with high transverse momentum, which is
reconstructed from a pair of opposite-sign same-flavor
leptons. Pair and single production of vectorlike quarks are
both taken into account and are each searched for using
optimized dileptonic exclusive and trileptonic inclusive
event selections. In these selections, the high scalar sum
of jet transverse momenta, the presence of
high-transverse-momentum large-radius jets, as well as - in
the case of the single-production selections - the presence
of forward jets are used. No significant excess over the
background-only hypothesis is found and exclusion limits at
95% confidence level allow masses of vectorlike quarks of
mT>1030 GeV (mT>1210 GeV) and mB>1010 GeV (mB>1140 GeV) in
the singlet (doublet) model. In the case of 100% branching
ratio for T→Zt (B→Zb), the limits are mT>1340 GeV
(mB>1220 GeV). Limits at 95% confidence level are also set
on the coupling to Standard Model quarks for given
vectorlike quark masses.},
Doi = {10.1103/PhysRevD.98.112010},
Key = {fds356636}
}
@article{fds307697,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale,
V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Caramarcu, C and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo
Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez,
AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai,
A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira,
AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini,
F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B and Clement, C and Clifft, RW},
Title = {Search for pair production of a heavy up-type quark decaying
to a W boson and a b quark in the lepton + jets channel with
the ATLAS detector.},
Journal = {Physical review letters},
Volume = {108},
Number = {26},
Pages = {261802},
Year = {2012},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.108.261802},
Abstract = {A search is presented for production of a heavy up-type
quark (t') together with its antiparticle, assuming
subsequent decay to a W boson and a b quark, t't[over
¯]'→W(+)bW(-)b[over ¯]. The search is based on 1.04
fb(-1) of proton-proton collisions at √[s]=7 TeV collected
by the ATLAS detector at the CERN Large Hadron Collider.
Data are analyzed in the lepton+jets final state,
characterized by a high transverse momentum isolated
electron or muon, high missing transverse momentum, and at
least three jets. No significant excess of events above the
background expectation is observed. A 95% C.L. lower limit
of 404 GeV is set for the mass of the t'
quark.},
Doi = {10.1103/physrevlett.108.261802},
Key = {fds307697}
}
@article{fds307690,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
Title = {Search for pair production of a new b' quark that decays
into a Z boson and a bottom quark with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {109},
Number = {7},
Pages = {071801},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.109.071801},
Abstract = {A search is reported for the pair production of a new quark
b' with at least one b' decaying to a Z boson and a bottom
quark. The data, corresponding to 2.0 fb(-1) of integrated
luminosity, were collected from pp collisions at √s = 7
TeV with the ATLAS detector at the CERN Large Hadron
Collider. Using events with a b-tagged jet and a Z boson
reconstructed from opposite-charge electrons, the mass
distribution of large transverse momentum b' candidates is
tested for an enhancement. No evidence for a b' signal is
detected in the observed mass distribution, resulting in the
exclusion at a 95% confidence level of b' quarks with masses
m (b') < 400 GeV that decay entirely via b' → Z+b. In the
case of a vectorlike singlet b' mixing solely with the third
standard model generation, masses m(b') < 358 GeV are
excluded.},
Doi = {10.1103/physrevlett.109.071801},
Key = {fds307690}
}
@article{fds313613,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G},
Title = {Search for pair production of a new heavy quark that decays
into a W boson and a light quark in pp collisions at s =8
TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {December},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.92.112007},
Abstract = {A search is presented for pair production of a new heavy
quark (Q) that decays into a W boson and a light quark (q)
in the final state where one W boson decays leptonically (to
an electron or muon plus a neutrino) and the other W boson
decays hadronically. The analysis is performed using an
integrated luminosity of 20.3 fb-1 of pp collisions at s=8
TeV collected by the ATLAS detector at the LHC. No evidence
of QQ¯ production is observed. New chiral quarks with
masses below 690 GeV are excluded at 95% confidence level,
assuming BR(Q→Wq)=1. Results are also interpreted in the
context of vectorlike quark models, resulting in the limits
on the mass of a vectorlike quark in the two-dimensional
plane of BR(Q→Wq) versus BR(Q→Hq).},
Doi = {10.1103/PhysRevD.92.112007},
Key = {fds313613}
}
@article{fds307855,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Ákesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Andeen, T and Anders, CF and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonelli, S and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S},
Title = {Search for pair production of first or second generation
leptoquarks in proton-proton collisions at √s=7TeV using
the ATLAS detector at the LHC},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {83},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.112006},
Abstract = {This paper describes searches for the pair production of
first or second generation scalar leptoquarks using 35pb-1
of proton-proton collision data recorded by the ATLAS
detector at √s=7TeV. Leptoquarks are searched in events
with two oppositely-charged muons or electrons and at least
two jets, and in events with one muon or electron, missing
transverse momentum and at least two jets. After event
selection, the observed yields are consistent with the
predicted backgrounds. Leptoquark production is excluded at
the 95 CL for masses MLQ<376 (319) GeV and MLQ<422 (362) GeV
for first and second generation scalar leptoquarks,
respectively, when assuming the branching fraction of a
leptoquark to a charged lepton is equal to 1.0 (0.5). ©
2011 American Physical Society.},
Doi = {10.1103/PhysRevD.83.112006},
Key = {fds307855}
}
@article{fds321111,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
A},
Title = {Search for pair production of gluinos decaying via stop and
sbottom in events with b -jets and large missing transverse
momentum in pp collisions at s =13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.032003},
Abstract = {A search for supersymmetry involving the pair production of
gluinos decaying via third-generation squarks to the
lightest neutralino (χ10) is reported. It uses an LHC
proton-proton data set at a center-of-mass energy s=13 TeV
with an integrated luminosity of 3.2 fb-1 collected with the
ATLAS detector in 2015. The signal is searched for in events
containing several energetic jets, of which at least three
must be identified as b jets, large missing transverse
momentum, and, potentially, isolated electrons or muons.
Large-radius jets with a high mass are also used to identify
highly boosted top quarks. No excess is found above the
predicted background. For χ10 masses below approximately
700 GeV, gluino masses of less than 1.78 TeV and 1.76 TeV
are excluded at the 95% C.L. in simplified models of the
pair production of gluinos decaying via sbottom and stop,
respectively. These results significantly extend the
exclusion limits obtained with the s=8 TeV data
set.},
Doi = {10.1103/PhysRevD.94.032003},
Key = {fds321111}
}
@article{fds307632,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JB and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
Costa, JJBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Bege, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Busey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua,
M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, JJ and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas,
CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, JJ and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A},
Title = {Search for pair production of heavy top-like quarks decaying
to a high-pT W boson and a b
quark in the lepton plus jets final state at √s=7
TeV with the ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {718},
Number = {4-5},
Pages = {1284-1302},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2012.11.071},
Abstract = {© 2012 CERN A search is presented for production of a heavy
up-type quark (t′) together with its antiparticle,
assuming a significant branching ratio for subsequent decay
into a W boson and a b quark. The search is based on 4.7
fb−1 of pp collisions at s=7 TeV recorded in 2011 with the
ATLAS detector at the CERN Large Hadron Collider. Data are
analyzed in the lepton + jets final state, characterized by
a high-transverse-momentum isolated electron or muon, large
missing transverse momentum and at least three jets. The
analysis strategy relies on the substantial boost of the W
bosons in the t′t¯′ signal when mt′≳400 GeV. No
significant excess of events above the Standard Model
expectation is observed and the result of the search is
interpreted in the context of fourth-generation and
vector-like quark models. Under the assumption of a
branching ratio BR(t′→Wb)=1, a fourth-generation t′
quark with mass lower than 656 GeV is excluded at 95%
confidence level. In addition, in light of the recent
discovery of a new boson of mass ∼126 GeV at the LHC,
upper limits are derived in the two-dimensional plane of
BR(t′→Wb) versus BR(t′→Ht), where H is the Standard
Model Higgs boson, for vector-like quarks of various
masses.},
Doi = {10.1016/j.physletb.2012.11.071},
Key = {fds307632}
}
@article{fds356667,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Search for pair production of heavy vector-like quarks
decaying into high-p T W bosons and top quarks in
the lepton-plus-jets final state in pp collisions at √s=13
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {8},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2018)048},
Abstract = {A search is presented for the pair production of heavy
vector-like B quarks, primarily targeting B quark decays
into a W boson and a top quark. The search is based on 36.1
fb−1 of pp collisions at s=13 TeV recorded in 2015 and
2016 with the ATLAS detector at the CERN Large Hadron
Collider. Data are analysed in the lepton-plus-jets final
state, characterised by a high-transverse-momentum isolated
electron or muon, large missing transverse momentum, and
multiple jets, of which at least one is b-tagged. No
significant deviation from the Standard Model expectation is
observed. The 95% confidence level lower limit on the B mass
is 1350 GeV assuming a 100% branching ratio to Wt. In the
SU(2) singlet scenario, the lower mass limit is 1170 GeV.
The 100% branching ratio limits are found to be also
applicable to heavy vector-like X production, with charge
+5/3, that decay into Wt. This search is also sensitive to a
heavy vector-like B quark decaying into other final states
(Zb and Hb) and thus mass limits on B production are set as
a function of the decay branching ratios.[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP08(2018)048},
Key = {fds356667}
}
@article{fds356733,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for pair production of heavy vector-like quarks
decaying to high-p T W bosons and b quarks in the
lepton-plus-jets final state in pp collisions at √s=13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {10},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2017)141},
Abstract = {A search is presented for the pair production of heavy
vector-like T quarks, primarily targeting the T quark decays
to a W boson and a b-quark. The search is based on 36.1
fb−1 of pp collisions at s=13 TeV recorded in 2015 and
2016 with the ATLAS detector at the CERN Large Hadron
Collider. Data are analysed in the lepton-plus-jets final
state, including at least one b-tagged jet and a
large-radius jet identified as originating from the hadronic
decay of a high-momentum W boson. No significant deviation
from the Standard Model expectation is observed in the
reconstructed T mass distribution. The observed 95%
confidence level lower limit on the T mass are 1350 GeV
assuming 100% branching ratio to Wb. In the SU(2) singlet
scenario, the lower mass limit is 1170 GeV. This search is
also sensitive to a heavy vector-like B quark decaying to Wt
and other final states. The results are thus reinterpreted
to provide a 95% confidence level lower limit on the B quark
mass at 1250 GeV assuming 100% branching ratio to Wt; in the
SU(2) singlet scenario, the limit is 1080 GeV. Mass limits
on both T and B production are also set as a function of the
decay branching ratios. The 100% branching ratio limits are
found to be applicable to heavy vector-like Y and X
production that decay to Wb and Wt, respectively.},
Doi = {10.1007/JHEP10(2017)141},
Key = {fds356733}
}
@article{fds356641,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Search for pair production of heavy vectorlike quarks
decaying into hadronic final states in pp collisions at s
=13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {9},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.98.092005},
Abstract = {A search is presented for the pair production of heavy
vectorlike quarks, TT or BB, that decay into final states
with jets and no reconstructed leptons. Jets in the final
state are classified using a deep neural network as arising
from hadronically decaying W/Z bosons, Higgs bosons, top
quarks, or background. The analysis uses data from the ATLAS
experiment corresponding to 36.1 fb-1 of proton-proton
collisions with a center-of-mass energy of s=13 TeV
delivered by the Large Hadron Collider in 2015 and 2016. No
significant deviation from the Standard Model expectation is
observed. Results are interpreted assuming the vectorlike
quarks decay into a Standard Model boson and a
third-generation-quark, T→Wb,Ht,Zt or B→Wt,Hb,Zb, for a
variety of branching ratios. At 95% confidence level, the
observed (expected) lower limit on the vectorlike B-quark
mass for a weak-isospin doublet (B, Y) is 950 (890) GeV, and
the lower limits on the masses for the pure decays B→Hb
and T→Ht, where these results are strongest, are 1010
(970) GeV and 1010 (1010) GeV, respectively.},
Doi = {10.1103/PhysRevD.98.092005},
Key = {fds356641}
}
@article{fds321100,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for pair production of Higgs bosons in the bbbb final
state using proton-proton collisions at √s =13 TeV with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.94.052002},
Abstract = {A search for Higgs-boson pair production in the bbbb final
state is carried out with 3.2 fb-1 of proton-proton
collision data collected at s=13 TeV with the ATLAS
detector. The data are consistent with the estimated
background and are used to set upper limits on the
production cross section of Higgs-boson pairs times
branching ratio to bbbb for both nonresonant and resonant
production. In the case of resonant production of
Kaluza-Klein gravitons within the Randall-Sundrum model,
upper limits in the 24 to 91 fb range are obtained for
masses between 600 and 3000 GeV, at the 95% confidence
level. The production cross section times branching ratio
for nonresonant Higgs-boson pairs is also constrained to be
less than 1.22 pb, at the 95% confidence
level.},
Doi = {10.1103/PhysRevD.94.052002},
Key = {fds321100}
}
@article{fds347449,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for pair production of Higgs bosons in the bb¯ bb¯
final state using proton-proton collisions at √s=13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {1},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2019)030},
Abstract = {A search for Higgs boson pair production in the bb¯ bb¯
final state is carried out with up to 36.1 fb−1 of LHC
proton-proton collision data collected at s=13 TeV with the
ATLAS detector in 2015 and 2016. Three benchmark signals are
studied: a spin-2 graviton decaying into a Higgs boson pair,
a scalar resonance decaying into a Higgs boson pair, and
Standard Model non-resonant Higgs boson pair production. Two
analyses are carried out, each implementing a particular
technique for the event reconstruction that targets Higgs
bosons reconstructed as pairs of jets or single boosted
jets. The resonance mass range covered is 260–3000 GeV.
The analyses are statistically combined and upper limits on
the production cross section of Higgs boson pairs times
branching ratio to bb¯ bb¯ are set in each model. No
significant excess is observed; the largest deviation of
data over prediction is found at a mass of 280 GeV,
corresponding to 2.3 standard deviations globally. The
observed 95% confidence level upper limit on the
non-resonant production is 13 times the Standard Model
prediction.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP01(2019)030},
Key = {fds347449}
}
@article{fds356642,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for pair production of Higgsinos in final states with
at least three b -tagged jets in s =13 TeV pp collisions
using the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {9},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.98.092002},
Abstract = {A search for pair production of the supersymmetric partners
of the Higgs boson (higgsinos H) in gauge-mediated scenarios
is reported. Each higgsino is assumed to decay to a Higgs
boson and a gravitino. Two complementary analyses, targeting
high- and low-mass signals, are performed to maximize
sensitivity. The two analyses utilize LHC pp collision data
at a center-of-mass energy s=13 TeV, the former with an
integrated luminosity of 36.1 fb-1 and the latter with 24.3
fb-1, collected with the ATLAS detector in 2015 and 2016.
The search is performed in events containing missing
transverse momentum and several energetic jets, at least
three of which must be identified as b-quark jets. No
significant excess is found above the predicted background.
Limits on the cross section are set as a function of the
mass of the H in simplified models assuming production via
mass-degenerate higgsinos decaying to a Higgs boson and a
gravitino. Higgsinos with masses between 130 and 230 GeV and
between 290 and 880 GeV are excluded at the 95% confidence
level. Interpretations of the limits in terms of the
branching ratio of the higgsino to a Z boson or a Higgs
boson are also presented, and a 45% branching ratio to a
Higgs boson is excluded for mH≈400 GeV.},
Doi = {10.1103/PhysRevD.98.092002},
Key = {fds356642}
}
@article{fds307663,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for pair production of massive particles decaying
into three quarks with the ATLAS detector in √s = 7 TeV pp
collisions at the LHC},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {12},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP12(2012)086},
Abstract = {A search is conducted for hadronic three-body decays of a
new massive coloured particle in √s = 7 TeV pp collisions
at the LHC using an integrated luminosity of 4.6 fb-1
collected by the ATLAS detector. Supersymmetric gluino pair
production in the context of a model with R-parity violation
is used as a benchmark scenario. The analysis is divided
into two search channels, each optimised separately for
their sensitivity to high-mass and low-mass gluino
production. The first search channel uses a stringent
selection on the transverse momentum of the six leading jets
and is performed as a counting experiment. The second search
channel focuses on low-mass gluinos produced with a large
boost. Large-radius jets are selected and the invariant mass
of each of the two leading jets is used as a discriminant
between the signal and the background. The results are found
to be consistent with Standard Model expectations and limits
are set on the allowed gluino mass.[Figure not available:
see fulltext.] © 2012 Cern for the benefit of the ATLAS
collaboration.},
Doi = {10.1007/JHEP12(2012)086},
Key = {fds307663}
}
@article{fds355954,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C},
Title = {Search for pair production of scalar leptoquarks decaying
into first- or second-generation leptons and top quarks in
proton–proton collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {4},
Year = {2021},
Month = {April},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09009-8},
Abstract = {A search for pair production of scalar leptoquarks, each
decaying into either an electron or a muon and a top quark,
is presented. This is the first leptoquark search using
ATLAS data to investigate top-philic cross-generational
couplings that could provide explanations for recently
observed anomalies in B meson decays. This analysis targets
high leptoquark masses which cause the decay products of
each resultant top quark to be contained within a single
high-pT large-radius jet. The full Run 2 dataset is
exploited, consisting of 139fb-1 of data collected from
proton–proton collisions at s=13TeV from 2015 to 2018 with
the ATLAS detector at the CERN Large Hadron Collider. In the
absence of any significant deviation from the background
expectation, lower limits on the leptoquark masses are set
at 1480GeV and 1470GeV for the electron and muon channel,
respectively.},
Doi = {10.1140/epjc/s10052-021-09009-8},
Key = {fds355954}
}
@article{fds307593,
Author = {Aaltonen, T and Albin, E and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Search for pair production of strongly interacting particles
decaying to pairs of jets in pp collisions at √s=1.96
TeV.},
Journal = {Physical review letters},
Volume = {111},
Number = {3},
Pages = {031802},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1103/physrevlett.111.031802},
Abstract = {We present a search for the pair production of a narrow
nonstandard-model strongly interacting particle that decays
to a pair of quarks or gluons, leading to a final state with
four hadronic jets. We consider both nonresonant production
via an intermediate gluon as well as resonant production via
a distinct nonstandard-model intermediate strongly
interacting particle. We use data collected by the CDF
experiment in proton-antiproton collisions at √[s]=1.96
TeV corresponding to an integrated luminosity of 6.6 fb(-1).
We find the data to be consistent with nonresonant
production. We report limits on σ(pp[over ¯]→jjjj) as a
function of the masses of the hypothetical intermediate
particles. Upper limits on the production cross sections for
nonstandard-model particles in several resonant and
nonresonant processes are also derived.},
Doi = {10.1103/physrevlett.111.031802},
Key = {fds307593}
}
@article{fds307902,
Author = {Aaltonen, and T, and others},
Title = {Search for Pair Production of Supersymmetric Top Quarks in
Dilepton Events from $p\bar{p}$ Collisions at $\sqrt{s}$ =
1.96 TeV},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {25},
Pages = {251801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.251801},
Abstract = {http://arxiv.org/abs/0912.1308},
Doi = {10.1103/PhysRevLett.104.251801},
Key = {fds307902}
}
@article{fds375364,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya,
BS and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Tamlihat, MA and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Flores, CAA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Estevez, MA and Fernandez, AA and Alviggi, MG and Aly, M and Coutinho, YA and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E},
Title = {Search for pair production of third-generation leptoquarks
decaying into a bottom quark and a τ -lepton with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {11},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-12104-7},
Abstract = {A search for pair-produced scalar or vector leptoquarks
decaying into a b-quark and a τ -lepton is presented using
the full LHC Run 2 (2015–2018) data sample of 139 fb - 1
collected with the ATLAS detector in proton–proton
collisions at a centre-of-mass energy of s=13 TeV. Events in
which at least one τ -lepton decays hadronically are
considered, and multivariate discriminants are used to
extract the signals. No significant deviations from the
Standard Model expectation are observed and 95%
confidence-level upper limits on the production
cross-section are derived as a function of leptoquark mass
and branching ratio B into a τ -lepton and b-quark. For
scalar leptoquarks, masses below 1460 GeV are excluded
assuming B= 100 %, while for vector leptoquarks the
corresponding limit is 1650 GeV (1910 GeV) in the
minimal-coupling (Yang–Mills) scenario.},
Doi = {10.1140/epjc/s10052-023-12104-7},
Key = {fds375364}
}
@article{fds357657,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler,
A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and An, F and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo, MA and Aperio
Bella, L and Aranzabal, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arguin, JF and Argyropoulos,
S},
Title = {Search for pair production of third-generation scalar
leptoquarks decaying into a top quark and a τ-lepton in pp
collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {6},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2021)179},
Abstract = {A search for pair production of third-generation scalar
leptoquarks decaying into a top quark and a τ-lepton is
presented. The search is based on a dataset of pp collisions
at s = 13 TeV recorded with the ATLAS detector during Run 2
of the Large Hadron Collider, corresponding to an integrated
luminosity of 139 fb−1. Events are selected if they have
one light lepton (electron or muon) and at least one
hadronically decaying τ -lepton, or at least two light
leptons. In addition, two or more jets, at least one of
which must be identified as containing b-hadrons, are
required. Six final states, defined by the multiplicity and
flavour of lepton candidates, are considered in the
analysis. Each of them is split into multiple event
categories to simultaneously search for the signal and
constrain several leading backgrounds. The signal-rich event
categories require at least one hadronically decaying
τ-lepton candidate and exploit the presence of energetic
final-state objects, which is characteristic of signal
events. No significant excess above the Standard Model
expectation is observed in any of the considered event
categories, and 95% CL upper limits are set on the
production cross section as a function of the leptoquark
mass, for different assumptions about the branching
fractions into tτ and bν. Scalar leptoquarks decaying
exclusively into tτ are excluded up to masses of 1.43 TeV
while, for a branching fraction of 50% into tτ, the lower
mass limit is 1.22 TeV. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP06(2021)179},
Key = {fds357657}
}
@article{fds336451,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Search for pair production of up-type vector-like quarks and
for four-top-quark events in final states with multiple
b-jets with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {7},
Publisher = {Springer Nature},
Year = {2018},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2018)089},
Abstract = {A search for pair production of up-type vector-like quarks
(T) with a significant branching ratio into a top quark and
either a Standard Model Higgs boson or a Z boson is
presented. The same analysis is also used to search for
four-top-quark production in several new physics scenarios.
The search is based on a dataset of pp collisions at s=13
TeV recorded in 2015 and 2016 with the ATLAS detector at the
CERN Large Hadron Collider and corresponds to an integrated
luminosity of 36.1 fb-1. Data are analysed in the
lepton+jets final state, characterised by an isolated
electron or muon with high transverse momentum, large
missing transverse momentum and multiple jets, as well as
the jets + ETmiss final state, characterised by multiple
jets and large missing transverse momentum. The search
exploits the high multiplicity of jets identified as
originating from b-quarks, and the presence of boosted,
hadronically decaying top quarks and Higgs bosons
reconstructed as large-radius jets, characteristic of signal
events. No significant excess above the Standard Model
expectation is observed, and 95% CL upper limits are set on
the production cross sections for the different signal
processes considered. These cross-section limits are used to
derive lower limits on the mass of a vector-like T quark
under several branching ratio hypotheses assuming
contributions from T ? W b, Zt, Ht decays. The 95% CL
observed lower limits on the T quark mass range between 0.99
TeV and 1.43 TeV for all possible values of the branching
ratios into the three decay modes considered, significantly
extending the reach beyond that of previous searches.
Additionally, upper limits on anomalous four-top-quark
production are set in the context of an effective field
theory model, as well as in an universal extra dimensions
model.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP07(2018)089},
Key = {fds336451}
}
@article{fds356745,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos,
SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for pair production of vector-like top quarks in
events with one lepton, jets, and missing transverse
momentum in √s=13 TeV pp collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {8},
Year = {2017},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2017)052},
Abstract = {The results of a search for vector-like top quarks using
events with exactly one lepton, at least four jets, and
large missing transverse momentum are reported. The search
is optimised for pair production of vector-like top quarks
in the Z() t + X decay channel. LHC pp collision data at a
centre-of-mass energy of s=13 TeV recorded by the ATLAS
detector in 2015 and 2016 are used, corresponding to an
integrated luminosity of 36.1 fb−1. No significant excess
over the Standard Model expectation is seen and upper limits
on the production cross-section of a vector-like T quark
pair as a function of the T quark mass are derived. The
observed (expected) 95% CL lower limits on the T mass are
870 GeV (890 GeV) for the weak-isospin singlet model, 1.05
TeV (1.06 TeV) for the weak-isospin doublet model and 1.16
TeV (1.17 TeV) for the pure Zt decay mode. Limits are also
set on the mass as a function of the decay branching ratios,
excluding large parts of the parameter space for masses
below 1 TeV.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP08(2017)052},
Key = {fds356745}
}
@article{fds307739,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for pair-produced heavy quarks decaying to Wq in the
two-lepton channel at √(s)=7TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.86.012007},
Abstract = {A search is presented for heavy-quark pair production (QQ̄)
under the decay hypothesis QQ̄→W+qW-q̄ with q=d, s, b
for up-type Q or q=u, c for down-type Q. The search is
performed with 1.04fb-1 of integrated luminosity from pp
collisions at √s=7TeV collected by the ATLAS detector at
the CERN LHC. Dilepton final states are selected, requiring
large missing transverse momentum and at least two jets.
Mass reconstruction of heavy-quark candidates is performed
by assuming that the W boson decay products are nearly
collinear. The data are in agreement with standard model
expectations; a heavy quark with mass less than 350 GeV is
excluded at 95% confidence level. © 2012 CERN. Published by
the American Physical Society under the terms of the
http://creativecommons.org/licenses/by/ 3.0/ Creative
Commons Attribution 3.0 License. Further distribution of
this work must maintain attribution to the author(s) and the
published article's title, journal citation, and
DOI.},
Doi = {10.1103/PhysRevD.86.012007},
Key = {fds307739}
}
@article{fds325305,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for pair-produced long-lived neutral particles
decaying to jets in the ATLAS hadronic calorimeter in pp
collisions at s=8TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {743},
Pages = {15-34},
Publisher = {Elsevier BV},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2015.02.015},
Abstract = {The ATLAS detector at the Large Hadron Collider at CERN is
used to search for the decay of a scalar boson to a pair of
long-lived particles, neutral under the Standard Model gauge
group, in 20.3fb-1 of data collected in proton-proton
collisions at s=8TeV. This search is sensitive to long-lived
particles that decay to Standard Model particles producing
jets at the outer edge of the ATLAS electromagnetic
calorimeter or inside the hadronic calorimeter. No
significant excess of events is observed. Limits are
reported on the product of the scalar boson production cross
section times branching ratio into long-lived neutral
particles as a function of the proper lifetime of the
particles. Limits are reported for boson masses from 100 GeV
to 900 GeV, and a long-lived neutral particle mass from 10
GeV to 150 GeV.},
Doi = {10.1016/j.physletb.2015.02.015},
Key = {fds325305}
}
@article{fds307649,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Dos Santos and SPA and Amorim,
A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E},
Title = {Search for pair-produced massive coloured scalars in
four-jet final states with the ATLAS detector in
proton–proton collisions at √s =7 TeV},
Journal = {European Physical Journal C},
Volume = {73},
Number = {1},
Pages = {1-20},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2263-z},
Abstract = {A search for pair-produced massive coloured scalar particles
decaying to a four-jet final state is performed by the ATLAS
experiment at the LHC in proton–proton collisions at √s
= 7 TeV. The analysed data sample corresponds to an
integrated luminosity of 4.6 fb<sup>−1</sup>. No deviation
from the Standard Model is observed in the invariant mass
spectrum of the two-jet pairs. A limit on the scalar gluon
pair production cross section of 70 pb (10 pb) is obtained
at the 95 % confidence level for a scalar gluon mass of 150
GeV (350 GeV). Interpreting these results as mass limits on
scalar gluons, masses ranging from 150 GeV to 287 GeV are
excluded at the 95 % confidence level.},
Doi = {10.1140/epjc/s10052-012-2263-z},
Key = {fds307649}
}
@article{fds310364,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for pair-produced third-generation squarks decaying
via charm quarks or in compressed supersymmetric scenarios
in pp collisions at √s =8TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052008},
Abstract = {Results of a search for supersymmetry via direct production
of third-generation squarks are reported, using 20.3fb-1 of
proton-proton collision data at s=8TeV recorded by the ATLAS
experiment at the LHC in 2012. Two different analysis
strategies based on monojetlike and c-tagged event
selections are carried out to optimize the sensitivity for
direct top squark-pair production in the decay channel to a
charm quark and the lightest neutralino (t∼1→c+χ∼10)
across the top squark-neutralino mass parameter space. No
excess above the Standard Model background expectation is
observed. The results are interpreted in the context of
direct pair production of top squarks and presented in terms
of exclusion limits in the (mt∼1, mχ∼10) parameter
space. A top squark of mass up to about 240 GeV is excluded
at 95% confidence level for arbitrary neutralino masses,
within the kinematic boundaries. Top squark masses up to 270
GeV are excluded for a neutralino mass of 200 GeV. In a
scenario where the top squark and the lightest neutralino
are nearly degenerate in mass, top squark masses up to 260
GeV are excluded. The results from the monojetlike analysis
are also interpreted in terms of compressed scenarios for
top squark-pair production in the decay channel
t∼1→b+ff′+χ∼10 and sbottom pair production with
b∼1→b+χ∼10, leading to a similar exclusion for nearly
mass-degenerate third-generation squarks and the lightest
neutralino. The results in this paper significantly extend
previous results at colliders.},
Doi = {10.1103/PhysRevD.90.052008},
Key = {fds310364}
}
@article{fds374026,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Search for pair-produced vector-like top and bottom partners
in events with large missing transverse momentum in pp
collisions with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {8},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11790-7},
Abstract = {A search for pair-produced vector-like quarks using events
with exactly one lepton (e or μ), at least four jets
including at least one b-tagged jet, and large missing
transverse momentum is presented. Data from proton–proton
collisions at a centre-of-mass energy of s= 13 TeV ,
recorded by the ATLAS detector at the LHC from 2015 to 2018
and corresponding to an integrated luminosity of 139 fb - 1
, are analysed. Vector-like partners T and B of the top and
bottom quarks are considered, as is a vector-like X with
charge + 5 / 3 , assuming their decay into a W, Z, or Higgs
boson and a third-generation quark. No significant
deviations from the Standard Model expectation are observed.
Upper limits on the production cross-section of T and B
quark pairs as a function of their mass are derived for
various decay branching ratio scenarios. The strongest lower
limits on the masses are 1.59 TeV assuming mass-degenerate
vector-like quarks and branching ratios corresponding to the
weak-isospin doublet model, and 1.47 TeV (1.46 TeV) for
exclusive T→ Zt (B/ X→ Wt) decays. In addition, lower
limits on the T and B quark masses are derived for all
possible branching ratios.},
Doi = {10.1140/epjc/s10052-023-11790-7},
Key = {fds374026}
}
@article{fds372125,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Search for pair-production of vector-like quarks in pp
collision events at s=13 TeV with at least one leptonically
decaying Z boson and a third-generation quark with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {843},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138019},
Abstract = {A search for the pair-production of vector-like quarks
optimized for decays into a Z boson and a third-generation
Standard Model quark is presented, using the full Run 2
dataset corresponding to 139fb−1 of pp collisions at
s=13TeV, collected in 2015–2018 with the ATLAS detector at
the Large Hadron Collider. The targeted final state is
characterized by the presence of a Z boson with high
transverse momentum, reconstructed from a pair of
same-flavour leptons with opposite-sign charges, as well as
by the presence of b-tagged jets and high-transverse-momentum
large-radius jets reconstructed from calibrated
smaller-radius jets. Events with exactly two or at least
three leptons are used, which are further categorized by the
presence of boosted W, Z, and Higgs bosons and top quarks.
The categorization is performed using a neural-network-based
boosted object tagger to enhance the sensitivity to signal
relative to the background. No significant excess above the
background expectation is observed and exclusion limits at
95% confidence level are set on the masses of the
vector-like partners T and B of the top and bottom quarks,
respectively. The limits depend on the branching ratio
configurations and, in the case of 100% branching ratio for
T→Zt and 100% branching ratio for B→Zb, this search sets
the most stringent limits to date, allowing mT>1.60TeV and
mB>1.42TeV, respectively.},
Doi = {10.1016/j.physletb.2023.138019},
Key = {fds372125}
}
@article{fds347451,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A},
Title = {Search for pairs of highly collimated photon-jets in pp
collisions at s =13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {99},
Number = {1},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.99.012008},
Abstract = {Results of a search for the pair production of photon-jets -
collimated groupings of photons - in the ATLAS detector at
the Large Hadron Collider are reported. Highly collimated
photon-jets can arise from the decay of new, highly boosted
particles that can decay to multiple photons collimated
enough to be identified in the electromagnetic calorimeter
as a single, photonlike energy cluster. Data from
proton-proton collisions at a center-of-mass energy of 13
TeV, corresponding to an integrated luminosity of 36.7 fb-1,
were collected in 2015 and 2016. Candidate photon-jet pair
production events are selected from those containing two
reconstructed photons using a set of identification criteria
much less stringent than that typically used for the
selection of photons, with additional criteria applied to
provide improved sensitivity to photon-jets. Narrow excesses
in the reconstructed diphoton mass spectra are searched for.
The observed mass spectra are consistent with the Standard
Model background expectation. The results are interpreted in
the context of a model containing a new, high-mass scalar
particle with narrow width, X, that decays into pairs of
photon-jets via new, light particles, a. Upper limits are
placed on the cross section times the product of branching
ratios σ×B(X→aa)×B(a→γγ)2 for 200 GeV<mX<2 TeV and
for ranges of ma from a lower mass of 100 MeV up to between
2 and 10 GeV, depending upon mX. Upper limits are also
placed on σ×B(X→aa)×B(a→3π0)2 for the same range of
mX and for ranges of ma from a lower mass of 500 MeV up to
between 2 and 10 GeV.},
Doi = {10.1103/PhysRevD.99.012008},
Key = {fds347451}
}
@article{fds373738,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman,
J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait
Tamlihat, M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Albouy,
GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Algren, M and Alhroob,
M and Ali, B and Ali, HMJ and Ali, S and Alibocus, SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen,
JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung,
C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos,
KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA},
Title = {Search for pairs of muons with small displacements in pp
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {846},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138172},
Abstract = {A search for new phenomena giving rise to pairs of opposite
electrically charged muons with impact parameters in the
millimeter range is presented, using 139 fb−1 of s=13 TeV
pp collision data from the ATLAS detector at the LHC. The
search targets the gap in coverage between existing searches
targeting final states with leptons with large displacement
and prompt leptons. No significant excess over the
background expectation is observed and exclusion limits are
set on the mass of long-lived scalar supersymmetric
muon-partners (smuons) with much lower lifetimes than
previously targeted by displaced muon searches. Smuon
lifetimes down to 1 ps are excluded for a smuon mass of 100
GeV, and smuon masses up to 520 GeV are excluded for a
proper lifetime of 10 ps, at 95% confidence level. Finally,
model-independent limits are set on the contribution from
new phenomena to the signal-region yields.},
Doi = {10.1016/j.physletb.2023.138172},
Key = {fds373738}
}
@article{fds353481,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Search for pairs of scalar leptoquarks decaying into quarks
and electrons or muons in √s = 13 TeV pp collisions with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2020)112},
Abstract = {A search for new-physics resonances decaying into a lepton
and a jet performed by the ATLAS experiment is presented.
Scalar leptoquarks pair-produced in pp collisions at s = 13
TeV at the Large Hadron Collider are considered using an
integrated luminosity of 139 fb−1, corresponding to the
full Run 2 dataset. They are searched for in events with two
electrons or two muons and two or more jets, including jets
identified as arising from the fragmentation of c- or
b-quarks. The observed yield in each channel is consistent
with the Standard Model background expectation. Leptoquarks
with masses below 1.8 TeV and 1.7 TeV are excluded in the
electron and muon channels, respectively, assuming a
branching ratio into a charged lepton and a quark of 100%,
with minimal dependence on the quark flavour. Upper limits
on the aforementioned branching ratio are also given as a
function of the leptoquark mass. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2020)112},
Key = {fds353481}
}
@article{fds354612,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Search for phenomena beyond the Standard Model in events
with large b-jet multiplicity using the ATLAS detector at
the LHC},
Journal = {European Physical Journal C},
Volume = {81},
Number = {1},
Year = {2021},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08730-0},
Abstract = {A search is presented for new phenomena in events
characterised by high jet multiplicity, no leptons
(electrons or muons), and four or more jets originating from
the fragmentation of b-quarks (b-jets). The search uses
139fb-1 of s = 13 TeV proton–proton collision data
collected by the ATLAS experiment at the Large Hadron
Collider during Run 2. The dominant Standard Model
background originates from multijet production and is
estimated using a data-driven technique based on an
extrapolation from events with low b-jet multiplicity to the
high b-jet multiplicities used in the search. No significant
excess over the Standard Model expectation is observed and
95% confidence-level limits that constrain simplified models
of R-parity-violating supersymmetry are determined. The
exclusion limits reach 950 GeV in top-squark mass in the
models considered.},
Doi = {10.1140/epjc/s10052-020-08730-0},
Key = {fds354612}
}
@article{fds356707,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Arnaez, O and Arnold, H},
Title = {Search for photonic signatures of gauge-mediated
supersymmetry in 13 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {97},
Number = {9},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.97.092006},
Abstract = {A search is presented for photonic signatures, motivated by
generalized models of gauge-mediated supersymmetry breaking.
This search makes use of proton-proton collision data at
√s = 13 TeV corresponding to an integrated luminosity of
36.1 fb-1 recorded by the ATLAS detector at the LHC, and it
explores models dominated by both strong and electroweak
production of supersymmetric partner states. Experimental
signatures incorporating an isolated photon and significant
missing transverse momentum are explored. These signatures
include events with an additional photon or additional jet
activity not associated with any specific underlying quark
flavor. No significant excess of events is observed above
the Standard Model prediction, and 95% confidence-level
upper limits of between 0.083 and 0.32 fb are set on the
visible cross section of contributions from physics beyond
the Standard Model. These results are interpreted in terms
of lower limits on the masses of gluinos, squarks, and
gauginos in the context of generalized models of
gauge-mediated supersymmetry, which reach as high as 2.3 TeV
for strongly produced and 1.3 TeV for weakly produced
supersymmetric partner pairs.},
Doi = {10.1103/PhysRevD.97.092006},
Key = {fds356707}
}
@article{fds313608,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for photonic signatures of gauge-mediated
supersymmetry in 8 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {January},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.92.072001},
Abstract = {A search is presented for photonic signatures motivated by
generalized models of gauge-mediated supersymmetry breaking.
This search makes use of 20.3 fb-1 of proton-proton
collision data at √s = 8 TeV recorded by the ATLAS
detector at the LHC, and explores models dominated by both
strong and electroweak production of supersymmetric partner
states. Four experimental signatures incorporating an
isolated photon and significant missing transverse momentum
are explored. These signatures include events with an
additional photon, lepton, b-quark jet, or jet activity not
associated with any specific underlying quark flavor. No
significant excess of events is observed above the Standard
Model prediction and model-dependent 95% confidence-level
exclusion limits are set.},
Doi = {10.1103/PhysRevD.92.072001},
Key = {fds313608}
}
@article{fds310299,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Search for production of an Υ (1 S) meson in association
with a W or Z boson using the full 1.96 TeV pp ¯ collision
data set at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.91.052011},
Abstract = {Production of the Υ(1S) meson in association with a vector
boson is a rare process in the standard model with a cross
section predicted to be below the sensitivity of the
Tevatron. Observation of this process could signify
contributions not described by the standard model or reveal
limitations with the current nonrelativistic
quantum-chromodynamic models used to calculate the cross
section. We perform a search for this process using the full
Run II data set collected by the CDF II detector
corresponding to an integrated luminosity of 9.4fb-1. The
search considers the Υ→μμ decay and the decay of the W
and Z bosons into muons and electrons. In these purely
leptonic decay channels, we observe one ΥW candidate with
an expected background of 1.2±0.5 events, and one ΥZ
candidate with an expected background of 0.1±0.1 events.
Both observations are consistent with the predicted
background contributions. The resulting upper limits on the
cross section for Υ+W/Z production are the most sensitive
reported from a single experiment and place restrictions on
potential contributions from non-standard-model
physics.},
Doi = {10.1103/PhysRevD.91.052011},
Key = {fds310299}
}
@article{fds307846,
Author = {Aaltonen, and T, and al, E},
Title = {Search for Production of Heavy Particles Decaying to Top
Quarks and Invisible Particles in $p\overline{p}$ Collisions
at $\sqrt{s}=1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. Lett.},
Volume = {106},
Number = {19},
Pages = {191801},
Publisher = {American Physical Society},
Year = {2011},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevLett.106.191801},
Abstract = {We present a search for a new particle T' decaying to top
quark via T' → t + X, where X is an invisible particle. In
a data sample with 4.8 fb(-1) of integrated luminosity
collected by the CDF II detector at Fermilab in pp
collisions with √s = 1.96 TeV, we search for pair
production of T' in the lepton + jets channel, pp → tt + X
+ X → ℓνbqq'b + X + X. We interpret our results
primarily in terms of a model where T' are exotic fourth
generation quarks and X are dark matter particles. Current
direct and indirect bounds on such exotic quarks restrict
their masses to be between 300 and 600 GeV/c2, the dark
matter particle mass being anywhere below m(T'). The data
are consistent with standard model expectations, and we set
95% confidence level limits on the generic production of
T'T' → tt + X + X. For the dark matter model we exclude T'
at 95% confidence level up to m(T') = 360 GeV/c2 for
m(X) ≤ 100 GeV/c2.},
Doi = {10.1103/PhysRevLett.106.191801},
Key = {fds307846}
}
@article{fds307701,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
N and Benhammou, Y and Benitez Garcia and JA and Benjamin, DP and Benoit,
M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B and Clement, C and Clifft, RW},
Title = {Search for production of resonant states in the photon-jet
mass distribution using pp collisions at √s=7 TeV
collected by the ATLAS detector.},
Journal = {Physical review letters},
Volume = {108},
Number = {21},
Pages = {211802},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.211802},
Abstract = {This Letter describes a model-independent search for the
production of new resonant states in photon+jet events in
2.11 fb(-1) of proton-proton collisions at √s=7 TeV. We
compare the photon+jet mass distribution to a background
model derived from data and find consistency with the
background-only hypothesis. Given the lack of evidence for a
signal, we set 95% credibility level limits on generic
Gaussian-shaped signals and on a benchmark excited-quark
(q*) model, excluding 2 TeV Gaussian resonances with cross
section times branching fraction times acceptance times
efficiency near 5 fb and excluding q* masses below 2.46 TeV,
respectively.},
Doi = {10.1103/physrevlett.108.211802},
Key = {fds307701}
}
@article{fds310268,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Search for production of vector-like quark pairs and of four
top quarks in the lepton-plus-jets final state in pp
collisions at √s = 8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2015)105},
Abstract = {A search for pair production of vector-like quarks, both
up-type (T) and down-type (B), as well as for four-top-quark
production, is presented. The search is based on pp
collisions at (Formula presented.) TeV recorded in 2012 with
the ATLAS detector at the CERN Large Hadron Collider and
corresponding to an integrated luminosity of 20.3 fb−1.
Data are analysed in the lepton-plus-jets final state,
characterised by an isolated electron or muon with high
transverse momentum, large missing transverse momentum and
multiple jets. Dedicated analyses are performed targeting
three cases: a T quark with significant branching ratio to a
W boson and a b-quark (TT¯→Wb+X), and both a T quark and
a B quark with significant branching ratio to a Higgs boson
and a third-generation quark (TT¯→Ht+XandBB¯→Hb+X
respectively). No significant excess of events above the
Standard Model expectation is observed, and 95% CL lower
limits are derived on the masses of the vector-like T and B
quarks under several branching ratio hypotheses assuming
contributions from T → Wb, Zt, Ht and B → Wt, Zb, Hb
decays. The 95% CL observed lower limits on the T quark mass
range between 715 GeV and 950 GeV for all possible values of
the branching ratios into the three decay modes, and are the
most stringent constraints to date. Additionally, the most
restrictive upper bounds on four-top-quark production are
set in a number of new physics scenarios.},
Doi = {10.1007/JHEP08(2015)105},
Key = {fds310268}
}
@article{fds310319,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca,
D and Cindro, V and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu,
S},
Title = {Search for production of [Formula: see text] resonances
decaying to a lepton, neutrino and jets in [Formula: see
text] collisions at [Formula: see text] TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {5},
Pages = {209},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3425-6},
Abstract = {A search is presented for narrow diboson resonances decaying
to [Formula: see text] or [Formula: see text] in the final
state where one [Formula: see text] boson decays
leptonically (to an electron or a muon plus a neutrino) and
the other [Formula: see text] boson decays hadronically. The
analysis is performed using an integrated luminosity of
20.3 fb[Formula: see text] of [Formula: see text]
collisions at [Formula: see text] TeV collected by the
ATLAS detector at the large hadron collider. No evidence for
resonant diboson production is observed, and resonance
masses below 700 and 1490 GeV are excluded at 95 %
confidence level for the spin-2 Randall-Sundrum bulk
graviton [Formula: see text] with coupling constant of 1.0
and the extended gauge model [Formula: see text] boson
respectively.},
Doi = {10.1140/epjc/s10052-015-3425-6},
Key = {fds310319}
}
@article{fds307547,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho,
Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Astbury, A and Atkinson, M and Atlay, NB and Auerbach, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma, Y and Baak, MA and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, S and Balek, P and Balli, F and Banas,
E and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow,
N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus,
R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battistin, M and Bauer, F and Bawa, HS and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belloni, A and Beloborodova, OL and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez
Garcia, JA and Benjamin, DP and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernard, C and Bernat,
P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertolucci, F and Besana, MI and Besjes, GJ and Bessidskaia, O and Besson, N and Bethke, S and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Bittner, B and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Bogaerts, JA and Bogdanchikov,
AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, G and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Bunse, M and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron,
D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canelli, F and Canepa,
A and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin,
V and Cheu, E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Christidi, IA and Chromek-Burckhart, D and Chu, ML and Chudoba,
J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
Title = {Search for quantum black hole production in
high-invariant-mass lepton+jet final states using pp
collisions at √s=8 TeV and the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {112},
Number = {9},
Pages = {091804},
Year = {2014},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.112.091804},
Abstract = {This Letter presents a search for quantum black-hole
production using 20.3 fb-1 of data collected with the ATLAS
detector in pp collisions at the LHC at √s = 8 TeV. The
quantum black holes are assumed to decay into a final state
characterized by a lepton (electron or muon) and a jet. In
either channel, no event with a lepton-jet invariant mass of
3.5 TeV or more is observed, consistent with the expected
background. Limits are set on the product of cross sections
and branching fractions for the lepton+jet final states of
quantum black holes produced in a search region for
invariant masses above 1 TeV. The combined 95% confidence
level upper limit on this product for quantum black holes
with threshold mass above 3.5 TeV is 0.18 fb. This limit
constrains the threshold quantum black-hole mass to be above
5.3 TeV in the model considered.},
Doi = {10.1103/physrevlett.112.091804},
Key = {fds307547}
}
@article{fds376311,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek,
L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V},
Title = {Search for quantum black hole production in lepton + jet
final states using proton-proton collisions at vs = 13 TeV
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {109},
Number = {3},
Year = {2024},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.109.032010},
Abstract = {A search for quantum black holes in electron + jet and muon
+ jet invariant mass spectra is performed with 140 fb-1 of
data collected by the ATLAS detector in proton-proton
collisions at √s = 13 TeV at the Large Hadron Collider.
The observed invariant mass spectrum of lepton + jet pairs
is consistent with Standard Model expectations. Upper limits
are set at 95% confidence level on the production cross
section times branching fractions for quantum black holes
decaying into a lepton and a quark in a search region with
invariant mass above 2.0 TeV. The resulting quantum black
hole lower mass threshold limit is 9.2 TeV in the
Arkani-Hamed-Dimopoulos-Dvali model, and 6.8 TeV in the
Randall-Sundrum model.},
Doi = {10.1103/PhysRevD.109.032010},
Key = {fds376311}
}
@article{fds308192,
Author = {Affolder, T and Akimoto, H and Akopian, A and Albrow, MG and Amaral, P and Amidei, D and Anikeev, K and Antos, J and Apollinari, G and Arisawa, T and Artikov, A and Asakawa, T and Ashmanskas, W and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Bailey, S and Barbaro, PD and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Belforte, S and Bell, WH and Bellettini, G and Bellinger, J and Benjamin, D and Bensinger, J and Beretvas, A and Berge, JP and Berryhill, J and Bhatti,
A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Blusk, SR and Bocci, A and Bodek, A and Bokhari, W and Bolla, G and Bonushkin, Y and Bortoletto, D and Boudreau,
J and Brandl, A and Brink, SVD and Bromberg, C and Brozovic, M and Brubaker, E and Bruner, N and Buckley-Geer, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Byon-Wagner, A and Byrum, KL and Cabrera, S and Calafiura, P and Campbell, M and Carithers, W and Carlson, J and Carlsmith, D and Caskey, W and Castro, A and Cauz, D and Cerri, A and Chan, AW and Chang, PS and Chang, PT and Chapman, J and Chen,
C and Chen, YC and Cheng, MT and Chertok, M and Chiarelli, G and Chirikov-Zorin, I and Chlachidze, G and Chlebana, F and Christofek,
L and Chu, ML and Chung, YS and Ciobanu, CI and Clark, AG and Connolly, A and Conway, J and Cordelli, M and Cranshaw, J and Cropp, R and Culbertson,
R and Dagenhart, D and D'Auria, S and DeJongh, F and Dell'Agnello, S and Dell'Orso, M and Demortier, L and Deninno, M and Derwent, PF and Devlin,
T and Dittmann, JR and Dominguez, A and Donati, S and Done, J and D'Onofrio, M and Dorigo, T and Eddy, N and Einsweiler, K and Elias, JE and Jr, EE and Erbacher, R and Errede, D and Errede, S and Fan, Q and Feild,
RG and Fernandez, JP and Ferretti, C and Field, RD and Fiori, I and Flaugher, B and Foster, GW and Franklin, M and Freeman, J and Friedman,
J and Fukui, Y and Furic, I and Galeotti, S and Gallas, A and Gallinaro, M and Gao, T and Garcia-Sciveres, M and Garfinkel, AF and Gatti, P and Gay, C and Gerdes, DW and Giannetti, P and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldstein, J and Gorelov, I and Goshaw,
AT and Gotra, Y and Goulianos, K and Green, C and Grim, G and Gris, P and Groer, L and Grosso-Pilcher, C and Guenther, M and Guillian, G and Costa, JGD and Haas, RM and Haber, C and Hahn, SR and Hall, C and Handa, T and Handler, R and Hao, W and Happacher, F and Hara, K and Hardman, AD and Harris, RM and Hartmann, F and Hatakeyama, K and Hauser, J and Heinrich,
J and Heiss, A and Herndon, M and Hill, C and Hoffman, KD and Holck, C and Hollebeek, R and Holloway, L and Hughes, R and Huston, J and Huth, J and Ikeda, H and Incandela, J and Introzzi, G and Iwai, J and Iwata, Y and James, E and Jones, M and Joshi, U and Kambara, H and Kamon, T and Kaneko,
T and Karr, K and Kasha, H and Kato, Y and Keaffaber, TA and Kelley, K and Kelly, M and Kennedy, RD and Kephart, R and Khazins, D and Kikuchi, T and Kilminster, B and Kim, BJ and Kim, DH and Kim, HS and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kirby, M and Kirk, M and Kirsch, L and Klimenko, S and Koehn, P and Kondo, K and Konigsberg, J and Korn, A and Korytov, A and Kotwal, AV and Kovacs, E and Kroll, J and Kruse, M and Kuhlmann, SE and Kurino, K and Kuwabara, T and Laasanen, AT and Lai, N and Lami, S and Lammel, S and Lancaster, J and Lancaster, M and Lander, R and Lath, A and Latino, G and LeCompte, T and IV, AML and Lee, K and Leone, S and Lewis,
JD and Lindgren, M and Liss, TM and Liu, JB and Liu, YC and Litvintsev, DO and Lobban, O and Lockyer, N and Loken, J and Loreti, M and Lucchesi, D and Lukens, P and Lusin, S and Lyons, L and Lys, J and Madrak, R and Maeshima,
K and Maksimovic, P and Malferrari, L and Mangano, M and Mariotti, M and Martignon, G and Martin, A and Matthews, JAJ and Mayer, J and Mazzanti,
P and McFarland, KS and McIntyre, P and McKigney, E and Menguzzato, M and Menzione, A and Mesropian, C and Meyer, A and Miao, T and Miller, R and Miller, JS and Minato, H and Miscetti, S and Mishina, M and Mitselmakher, G and Moggi, N and Moore, E and Moore, R and Morita, Y and Moulik, T and Mulhearn, M and Mukherjee, A and Muller, T and Munar, A and Murat, P and Murgia, S and Nachtman, J and Nagaslaev, V and Nahn, S and Nakada, H and Nakano, I and Nelson, C and Nelson, T and Neu, C and Neuberger, D and Newman-Holmes, C and Ngan, CYP and Niu, H and Nodulman,
L and Nomerotski, A and Oh, SH and Oh, YD and Ohmoto, T and Ohsugi, T and Oishi, R and Okusawa, T and Olsen, J and Orejudos, W and Pagliarone, C and Palmonari, F and Paoletti, R and Papadimitriou, V and Partos, D and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, D and Pescara, L and Phillips, TJ and Piacentino, G and Pitts, KT and Pompos,
A and Pondrom, L and Pope, G and Popovic, M and Prokoshin, F and Proudfoot,
J and Ptohos, F and Pukhov, O and Punzi, G and Rakitine, A and Ratnikov, F and Reher, D and Reichold, A and Ribon, A and Riegler, W and Rimondi, F and Ristori, L and Riveline, M and Robertson, WJ and Robinson, A and Rodrigo, T and Rolli, S and Rosenson, L and Roser, R and Rossin, R and Rott, C and Roy, A and Ruiz, A and Safonov, A and Denis, RS and Sakumoto,
WK and Saltzberg, D and Sanchez, C and Sansoni, A and Santi, L and Sato, H and Savard, P and Schlabach, P and Schmidt, EE and Schmidt, MP and Schmitt,
M and Scodellaro, L and Scott, A and Scribano, A and Segler, S and Seidel,
S and Seiya, Y and Semenov, A and Semeria, F and Shah, T and Shapiro, MD and Shepard, PF and Shibayama, T and Shimojima, M and Shochet, M and Sidoti,
A and Siegrist, J and Sill, A and Sinervo, P and Singh, P and Slaughter,
AJ and Sliwa, K and Smith, C and Snider, FD and Solodsky, A and Spalding,
J and Speer, T and Sphicas, P and Spinella, F and Spiropulu, M and Spiegel,
L and Steele, J and Stefanini, A and Strologas, J and Strumia, F and Stuart, D and Sumorok, K and Suzuki, T and Takano, T and Takashima, R and Takikawa, K and Tamburello, P and Tanaka, M and Tannenbaum, B and Tecchio, M and Tesarek, R and Teng, PK and Terashi, K and Tether, S and Thompson, AS and Thurman-Keup, R and Tipton, P and Tkaczyk, S and Toback, D and Tollefson, K and Tollestrup, A and Tonelli, D and Toyoda,
H and Trischuk, W and Troconiz, JFD and Tseng, J and Turini, N and Ukegawa,
F and Vaiciulis, T and Valls, J and III, SV and Velev, G and Veramendi, G and Vidal, R and Vila, I and Vilar, R and Volobouev, I and Mey, MVD and Vucinic, D and Wagner, RG and Wagner, RL and Wallace, NB and Wan, Z and Wang, C and Wang, MJ and Ward, B and Waschke, S and Watanabe, T and Waters,
D and Watts, T and Webb, R and Wenzel, H and III, WCW and Wicklund, AB and Wicklund, E and Wilkes, T and Williams, HH and Wilson, P and Winer, BL and Winn, D and Wolbers, S and Wolinski, D and Wolinski, J and Wolinski, S and Worm, S and Wu, X and Wyss, J and Yao, W and Yeh, GP and Yeh, P and Yoh, J and Yosef, C and Yoshida, T and Yu, I and Yu, S and Yu, Z and Zanetti, A and Zetti, F and Zucchelli, S},
Title = {Search for quark-lepton compositeness and a heavy W′ Boson
using the eν channel in pp̄ Collisions at √s = 1.8
TeV},
Journal = {Physical Review Letters},
Volume = {87},
Number = {23},
Pages = {2318031-2318036},
Year = {2001},
Month = {Winter},
ISSN = {0031-9007},
url = {http://www.ncbi.nlm.nih.gov/pubmed/11736446},
Abstract = {A study on searches for quark-lepton compositeness and a
heavy boson at high electron-neutrino transverse mass was
presented. The data collected in pp̄ collisions at √s=1.8
TeV was used for the analysis. The data obtained is found to
be consistent with the standard model (SM)
predictions.},
Doi = {10.1103/physrevlett.87.231803},
Key = {fds308192}
}
@article{fds331392,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk,
HE and Fisyak, Y and Flattum, E},
Title = {Search for R-parity violating supersymmetry in the
dielectron channel},
Journal = {Physical Review Letters},
Volume = {83},
Number = {22},
Pages = {4476-4481},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.83.4476},
Abstract = {We report on a search for R-parity-violating supersymmetry
in pp¯ collisions at √=1.8TeV using the D0 detector at
Fermilab. Events with at least two electrons and four or
more jets were studied. We observe two events in
99±4.4pb−1 of data, consistent with the expected
background of 1.8±0.4 events. This result is interpreted
within the framework of minimal low-energy supergravity
supersymmetry models. Squarks with mass below 243 GeV/c2 and
gluinos with mass below 227GeV/c2 are excluded at the 95%
C.L. for A0 = 0, μ<0, tan β=2, and a finite value for any
one of the six R-parity-violating couplings λ′1jk (j=1, 2
and k=1, 2, 3). © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.83.4476},
Key = {fds331392}
}
@article{fds308170,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR and Duperrin, A and Dyshkant, A and Edmunds, D and Ellison, J and Eltzroth, JT and Elvira, VD and Engelmann,
R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein, D and Ferbel, T and Filthaut, F and Fisk, HE and Fisyak, Y and Flattum, E and Fleuret, F and Fortner, M and Fox, H and Frame, KC and Fu, S and Fuess, S and Gallas, E and Galyaev, AN and Gao, M and Gavrilov, V and Genik, RJ and Genser, K and Gerber, CE and Gershtein, Y and Gilmartin, R and Ginther,
G and Gómez, B and Gómez, G and Goncharov, PI and González Solís,
JL and Gordon, H and Goss, LT and Gounder, K and Goussiou, A and Graf, N and Graham, G and Grannis, PD and Green, JA and Greenlee, H and Greenwood,
ZD and Grinstein, S and Groer, L and Grünendahl, S and Gupta, A and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Hadley, NJ and Haggerty, H and Hagopian, S and Hagopian, V and Hall, RE and Hanlet, P and Hansen, S and Hauptman, JM and Hays, C and Hebert, C and Hedin, D and Heinmiller, JM and Heinson, AP and Heintz, U and Hildreth, MD and Hirosky, R and Hobbs, JD and Hoeneisen, B and Huang, Y and Iashvili, I and Illingworth, R and Ito, AS and Jaffré, M and Jain, S and Jesik, R and Johns, K and Johnson, M and Jonckheere, A and Jöstlein, H and Juste, A and Kahl, W and Kahn, S and Kajfasz, E and Kalinin, AM and Karmanov, D and Karmgard, D and Kehoe, R and Khanov, A and Kharchilava, A and Kim, SK and Klima, B and Knuteson, B and Ko, W and Kohli, JM and Kostritskiy, AV and Kotcher, J and Kothari, B and Kotwal, AV and Kozelov, AV and Kozlovsky,
EA and Krane, J and Krishnaswamy, MR and Krivkova, P and Krzywdzinski,
S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kuznetsov, VE and Landsberg, G and Lee, WM and Leflat, A and Leggett, C and Lehner, F and Leonidopoulos, C and Li, J and Li, QZ and Li, X and Lima,
JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipton, R and Lucotte,
A and Lueking, L and Lundstedt, C and Luo, C and Maciel, AKA and Madaras,
RJ and Malyshev, VL and Manankov, V and Mao, HS and Marshall, T and Martin,
MI and Mauritz, KM and Mayorov, AA and McCarthy, R and McMahon, T and Melanson, HL and Merkin, M and Merritt, KW and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mokhov, N and Mondal, NK and Montgomery,
HE and Moore, RW and Mostafa, M and Da Motta and H and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret,
JP and Negroni, S and Nunnemann, T and O'Neil, D and Oguri, V and Olivier,
B and Oshima, N and Padley, P and Pan, LJ and Papageorgiou, K and Para, A and Parashar, N and Partridge, R and Parua, N and Paterno, M and Patwa, A and Pawlik, B and Perkins, J and Peters, O and Pétroff, P and Piegaia, R and Pope, BG and Popkov, E and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Raja, R and Rajagopalan, S and Ramberg,
E and Rapidis, PA and Reay, NW and Reucroft, S and Ridel, M and Rijssenbeek, M and Rizatdinova, F and Rockwell, T and Roco, M and Royon,
C and Rubinov, P and Ruchti, R and Rutherfoord, J and Sabirov, BM and Sajot, G and Santoro, A and Sawyer, L and Schamberger, RD and Schellman,
H and Schwartzman, A and Sen, N and Shabalina, E and Shivpuri, RK and Shpakov, D and Shupe, M and Sidwell, RA and Simak, V and Singh, H and Singh, JB and Sirotenko, V and Slattery, P and Smith, E and Smith, RP and Snihur, R and Snow, GR and Snow, J and Snyder, S and Solomon, J and Song,
Y and Sorín, V and Sosebee, M and Sotnikova, N and Soustruznik, K and Souza, M and Stanton, NR and Steinbrück, G and Stephens, RW and Stichelbaut, F and Stoker, D and Stolin, V and Stone, A and Stoyanova,
DA and Strang, MA and Strauss, M and Strovink, M and Stutte, L and Sznajder, A and Talby, M and Taylor, W and Tentindo-Repond, S and Tripathi, SM and Trippe, TG and Turcot, AS and Tuts, PM and Vaniev, V and Van Kooten and R and Varelas, N and Vertogradov, LS and Villeneuve-Seguier, F and Volkov, AA and Vorobiev, AP and Wahl, HD and Wang, H and Wang, Z-M and Warchol, J and Watts, G and Wayne, M and Weerts,
H and White, A and White, JT and Whiteson, D and Wijngaarden, DA and Willis, S and Wimpenny, SJ and Womersley, J and Wood, DR and Xu, Q and Yamada, R and Yamin, P and Yasuda, T and Yatsunenko, YA and Yip, K and Youssef, S and Yu, J and Yu, Z and Zanabria, M and Zhang, X and Zheng, H and Zhou, B and Zhou, Z and Zielinski, M and Zieminska, D and Zieminski, A and Zutshi, V and Zverev, EG and Zylberstejn, A},
Title = {Search for R-parity violating supersymmetry in two-muon and
four-jet topologies.},
Journal = {Physical review letters},
Volume = {89},
Number = {17},
Pages = {171801},
Year = {2002},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.89.171801},
Abstract = {We present results of a search for R-parity-violating decay
of the neutralino chi;01, taken as the lightest
supersymmetric particle, to a muon and two jets. The decay
proceeds through a lepton-number violating coupling
lambda(')(2jk) (j=1,2; k=1,2,3), with R-parity conservation
in all other production and decay processes. In the absence
of candidate events from 77.5+/-3.9 pb(-1) of data collected
by the D0 experiment at the Fermilab Tevatron in pp
collisions at sqrt[s]=1.8 TeV, and with an expected
background of 0.18+/-0.03+/-0.02 events, we set limits on
squark and gluino masses within the framework of the minimal
low-energy supergravity-supersymmetry model.},
Doi = {10.1103/physrevlett.89.171801},
Key = {fds308170}
}
@article{fds308204,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl,
OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov,
D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann,
R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
D},
Title = {Search for R-parity violation in multilepton final states in
[formula presented] collisions at [formula
presented]},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {62},
Number = {7},
Pages = {5},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.62.071701},
Abstract = {The result of a search for gaugino pair production with a
trilepton signature is reinterpreted in the framework of
minimal supergravity (MSUGRA) with R-parity violation via
leptonic λ Yukawa couplings. The search used 95 (Formula
presented) of (Formula presented) collisions at (Formula
presented) recorded by the DØ detector at the Fermilab
Tevatron. A large domain of the MSUGRA parameter space is
excluded for (Formula presented) (Formula presented). ©
2000 The American Physical Society.},
Doi = {10.1103/PhysRevD.62.071701},
Key = {fds308204}
}
@article{fds356652,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G},
Title = {Search for R-parity-violating supersymmetric particles in
multi-jet final states produced in p–p collisions at s=13
TeV using the ATLAS detector at the LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {785},
Pages = {136-158},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2018.08.021},
Abstract = {Results of a search for gluino pair production with
subsequent R-parity-violating decays to quarks are
presented. This search uses 36.1 fb−1 of data collected by
the ATLAS detector in proton–proton collisions with a
centre-of-mass energy of s=13 TeV at the LHC. The analysis
is performed using requirements on the number of jets and
the number of jets tagged as containing a b-hadron as well
as a topological observable formed by the scalar sum of
masses of large-radius jets in the event. No significant
excess above the expected Standard Model background is
observed. Limits are set on the production of gluinos in
models with the R-parity-violating decays of either the
gluino itself (direct decay) or the neutralino produced in
the R-parity-conserving gluino decay (cascade decay). In the
gluino cascade decay model, gluino masses below 1850 GeV are
excluded for 1000 GeV neutralino mass. For the gluino direct
decay model, the 95% confidence level upper limit on the
cross section times branching ratio varies between 0.80 fb
at mg˜=900 GeV and 0.011 fb at mg˜=1800
GeV.},
Doi = {10.1016/j.physletb.2018.08.021},
Key = {fds356652}
}
@article{fds359998,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
ATH and Arena, E and Arguin, JF and Argyropoulos, S and Arling,
JH},
Title = {Search for R-parity-violating supersymmetry in a final state
containing leptons and many jets with the ATLAS experiment
using √s=13TeV proton–proton collision
data},
Journal = {European Physical Journal C},
Volume = {81},
Number = {11},
Year = {2021},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09761-x},
Abstract = {A search for R-parity-violating supersymmetry in final
states characterized by high jet multiplicity, at least one
isolated light lepton and either zero or at least three
b-tagged jets is presented. The search uses 139fb-1 of
s=13TeV proton–proton collision data collected by the
ATLAS experiment during Run 2 of the Large Hadron Collider.
The results are interpreted in the context of
R-parity-violating supersymmetry models that feature gluino
production, top-squark production, or electroweakino
production. The dominant sources of background are estimated
using a data-driven model, based on observables at medium
jet multiplicity, to predict the b-tagged jet multiplicity
distribution at the higher jet multiplicities used in the
search. Machine-learning techniques are used to reach
sensitivity to electroweakino production, extending the
data-driven background estimation to the shape of the
machine-learning discriminant. No significant excess over
the Standard Model expectation is observed and exclusion
limits at the 95% confidence level are extracted, reaching
as high as 2.4 TeV in gluino mass, 1.35 TeV in top-squark
mass, and 320 (365) GeV in higgsino (wino)
mass.},
Doi = {10.1140/epjc/s10052-021-09761-x},
Key = {fds359998}
}
@article{fds307664,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for R-parity-violating supersymmetry in events with
four or more leptons in √s =7 TeV pp collisions with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {12},
Publisher = {Springer Nature},
Year = {2012},
Month = {December},
url = {http://dx.doi.org/10.1007/JHEP12(2012)124},
Abstract = {A search for new phenomena in final states with four or more
leptons (electrons or muons) is presented. The analysis is
based on 4.7 fb-1 of √s =7 TeV proton-proton collisions
delivered by the Large Hadron Collider and recorded with the
ATLAS detector. Observations are consistent with Standard
Model expectations in two signal regions: one that requires
moderate values of missing transverse momentum and another
that requires large effective mass. The results are
interpreted in a simplified model of R-parity-violating
supersymmetry in which a 95% CL exclusion region is set for
charged wino masses up to 540 GeV. In an R-parity-violating
MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are
excluded for 10 < tan β < 40. © 2012 Cern for the benefit
of the ATLAS collaboration.},
Doi = {10.1007/JHEP12(2012)124},
Key = {fds307664}
}
@article{fds356534,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Search for resonances decaying into a weak vector boson and
a Higgs boson in the fully hadronic final state produced in
proton-proton collisions at s =13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {102},
Number = {11},
Year = {2020},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.102.112008},
Abstract = {A search for heavy resonances decaying into a W or Z boson
and a Higgs boson produced in proton-proton collisions at
the Large Hadron Collider at s=13 TeV is presented. The
analysis utilizes the dominant W→qq¯′ or Z→qq¯ and
H→bb¯ decays with substructure techniques applied to
large-radius jets. A sample corresponding to an integrated
luminosity of 139 fb-1 collected with the ATLAS detector is
analyzed and no significant excess of data is observed over
the background prediction. The results are interpreted in
the context of the heavy vector triplet model with spin-1
W′ and Z′ bosons. Upper limits on the cross section are
set for resonances with mass between 1.5 and 5.0 TeV,
ranging from 6.8 to 0.53 fb for W′→WH and from 8.7 to
0.53 fb for Z′→ZH at the 95% confidence
level.},
Doi = {10.1103/PhysRevD.102.112008},
Key = {fds356534}
}
@article{fds307644,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for resonances decaying into top-quark pairs using
fully hadronic decays in pp collisions with ATLAS at √s=7
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {1},
Publisher = {Springer Nature},
Year = {2013},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP01(2013)116},
Abstract = {A search for resonances produced in 7 TeV proton-proton
collisions and decaying into top-quark pairs is described.
In this Letter events where the top-quark decay produces two
massive jets with large transverse momenta recorded with the
ATLAS detector at the Large Hadron Collider are considered.
Two techniques that rely on jet substructure are used to
separate top-quark jets from those arising from light quarks
and gluons. In addition, each massive jet is required to
have evidence of an associated bottom-quark decay. The data
are consistent with the Standard Model, and limits can be
set on the production cross section times branching fraction
of a Z′ boson and a Kaluza-Klein gluon resonance. These
limits exclude, at the 95% credibility level, Z′ bosons
with masses 0.70-1.00 TeV as well as 1.28-1.32 TeV and
Kaluza-Klein gluons with masses 0.70-1.62 TeV. © 2013 Cern
for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP01(2013)116},
Key = {fds307644}
}
@article{fds310264,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Anzà, F and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bianchi, L and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau,
J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian,
I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino,
G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos,
F and Punzi, G and Redondo Fernández and I and Renton, P and Rescigno, M and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St
Denis, R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Search for Resonances Decaying to Top and Bottom Quarks with
the CDF Experiment.},
Journal = {Physical review letters},
Volume = {115},
Number = {6},
Pages = {061801},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.115.061801},
Abstract = {We report on a search for charged massive resonances
decaying to top (t) and bottom (b) quarks in the full data
set of proton-antiproton collisions at a center-of-mass
energy of √[s]=1.96 TeV collected by the CDF II
detector at the Tevatron, corresponding to an integrated
luminosity of 9.5 fb(-1). No significant excess above
the standard model background prediction is observed. We set
95% Bayesian credibility mass-dependent upper limits on the
heavy charged-particle production cross section times
branching ratio to tb. Using a standard model extension with
a W'→tb and left-right-symmetric couplings as a benchmark
model, we constrain the W' mass and couplings in the
300-900 GeV/c(2) range. The limits presented here are
the most stringent for a charged resonance with mass in the
range 300-600 GeV/c(2) decaying to top and bottom
quarks.},
Doi = {10.1103/physrevlett.115.061801},
Key = {fds310264}
}
@article{fds321091,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Search for resonances in diphoton events at √s=13 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)001},
Abstract = {Searches for new resonances decaying into two photons in the
ATLAS experiment at the CERN Large Hadron Collider are
described. The analysis is based on proton-proton collision
data corresponding to an integrated luminosity of 3.2 fb−1
at s=13 TeV recorded in 2015. Two searches are performed,
one targeted at a spin-2 particle of mass larger than 500
GeV, using Randall-Sundrum graviton states as a benchmark
model, and one optimized for a spin-0 particle of mass
larger than 200 GeV. Varying both the mass and the decay
width, the most significant deviation from the
background-only hypothesis is observed at a diphoton
invariant mass around 750 GeV with local significances of
3.8 and 3.9 standard deviations in the searches optimized
for a spin-2 and spin-0 particle, respectively. The global
significances are estimated to be 2.1 standard deviations
for both analyses. The consistency between the data
collected at 13 TeV and 8 TeV is also evaluated. Limits on
the production cross section times branching ratio to two
photons for the two resonance types are reported.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP09(2016)001},
Key = {fds321091}
}
@article{fds356671,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Search for resonances in the mass distribution of jet pairs
with one or two jets identified as b -jets in proton-proton
collisions at s =13 TeV with the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {3},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.98.032016},
Abstract = {A search for new resonances decaying into jets containing
b-hadrons in pp collisions with the ATLAS detector at the
LHC is presented in the dijet mass range from 0.57 to 7 TeV.
The data set corresponds to an integrated luminosity of up
to 36.1 fb-1 collected in 2015 and 2016 at s=13 TeV. No
evidence of a significant excess of events above the smooth
background shape is found. Upper cross-section limits and
lower limits on the corresponding signal mass parameters for
several types of signal hypotheses are provided at 95% C.L.
In addition, 95% C.L. upper limits are set on the cross
sections for new processes that would produce
Gaussian-shaped signals in the di-b-jet mass
distributions.},
Doi = {10.1103/PhysRevD.98.032016},
Key = {fds356671}
}
@article{fds321131,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for resonances in the mass distribution of jet pairs
with one or two jets identified as b-jets in proton–proton
collisions at s=13 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {759},
Pages = {229-246},
Publisher = {Elsevier BV},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2016.05.064},
Abstract = {Searches for high-mass resonances in the dijet invariant
mass spectrum with one or two jets identified as b-jets are
performed using an integrated luminosity of 3.2 fb−1 of
proton–proton collisions with a centre-of-mass energy of
s=13 TeV recorded by the ATLAS detector at the Large Hadron
Collider. No evidence of anomalous phenomena is observed in
the data, which are used to exclude, at 95% credibility
level, excited b⁎ quarks with masses from 1.1 TeV to 2.1
TeV and leptophobic Z′ bosons with masses from 1.1 TeV to
1.5 TeV. Contributions of a Gaussian signal shape with
effective cross sections ranging from approximately 0.4 to
0.001 pb are also excluded in the mass range 1.5–5.0
TeV.},
Doi = {10.1016/j.physletb.2016.05.064},
Key = {fds321131}
}
@article{fds347454,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, J-F and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Baines, JT and Bajic,
M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas,
E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisits, M-S and Barkeloo, J and Barklow, T and Barlow, N and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous, S and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall, A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner,
M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RMB and Biebel, O and Biedermann, D and Bielski,
R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz,
T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black,
KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein,
U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson,
BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá,
S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
CH and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung,
K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou,
V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
IA},
Title = {Search for Resonant and Nonresonant Higgs Boson Pair
Production in the bb[over ¯]τ^{+}τ^{-} Decay Channel in
pp Collisions at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {121},
Number = {19},
Pages = {191801},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.121.191801},
Abstract = {A search for resonant and nonresonant pair production of
Higgs bosons in the bb[over ¯]τ^{+}τ^{-} final state is
presented. The search uses 36.1 fb^{-1} of pp collision
data with sqrt[s]=13 TeV recorded by the ATLAS
experiment at the LHC in 2015 and 2016. Decays of the
τ-lepton pairs with at least one τ lepton decaying to
final states with hadrons and a neutrino are considered. No
significant excess above the expected background is observed
in the data. The cross-section times branching ratio for
nonresonant Higgs boson pair production is constrained to be
less than 30.9 fb, 12.7 times the standard model
expectation, at 95% confidence level. The data are also
analyzed to probe resonant Higgs boson pair production,
constraining a model with an extended Higgs sector based on
two doublets and a Randall-Sundrum bulk graviton model.
Upper limits are placed on the resonant Higgs boson pair
production cross-section times branching ratio, excluding
resonances X in the mass range 305 GeV<m_{X}<402 GeV
in the simplified hMSSM minimal supersymmetric model for
tanβ=2 and excluding bulk Randall-Sundrum gravitons G_{KK}
in the mass range 325 GeV<m_{G_{KK}}<885 GeV for
k/M[over ¯]_{Pl}=1.},
Doi = {10.1103/physrevlett.121.191801},
Key = {fds347454}
}
@article{fds307595,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Search for resonant diboson production in the WW/WZ →
ℓvjj decay channels with the ATLAS detector at √s = 7
TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.87.112006},
Abstract = {A search for resonant diboson production using a data sample
corresponding to 4:7 fb–1of integrated luminosity
collected by the ATLAS experiment at the Large Hadron
Collider in pp collisions at √s = 7 TeV is presented. The
search for a narrow resonance in the WW or WZ mass
distribution is conducted in a final state with an electron
or a muon, missing transverse momentum, and at least two
jets. No significant excess is observed and limits are set
using three benchmark models: WW resonance masses below 940
and 710 GeV are excluded at 95% confidence level for spin-2
Randall–Sundrum and bulk Randall–Sundrum gravitons,
respectively; WZ resonance masses below 950 GeV are excluded
at 95% confidence level for a spin-1 extended gauge model
W′ boson.},
Doi = {10.1103/PhysRevD.87.112006},
Key = {fds307595}
}
@article{fds346165,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro,
A},
Title = {Search for resonant diboson production in the [Formula: see
text] final state in [Formula: see text] collisions at
[Formula: see text] TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {2},
Pages = {69},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3261-8},
Abstract = {This paper reports on a search for narrow resonances in
diboson production in the [Formula: see text] final state
using [Formula: see text] collision data corresponding to an
integrated luminosity of [Formula: see text] fb[Formula:
see text] collected at [Formula: see text] TeV with the
ATLAS detector at the Large Hadron Collider. No significant
excess of data events over the Standard Model expectation is
observed. Upper limits at the 95 % confidence level are set
on the production cross section times branching ratio for
Kaluza-Klein gravitons predicted by the Randall-Sundrum
model and for Extended Gauge Model [Formula: see text]
bosons. These results lead to the exclusion of mass values
below 740 and 1590 GeV for the graviton and [Formula: see
text] boson respectively.},
Doi = {10.1140/epjc/s10052-015-3261-8},
Key = {fds346165}
}
@article{fds307871,
Author = {Aaltonen, TEA},
Title = {Search for resonant production of $t\overline{t}$ decaying
to jets in $p\overline{p}$ collisions at
$\sqrt{s}\mathbf{=}1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.84.072003},
Abstract = {This paper reports a search for nonstandard model topquark
resonances, Z′, decaying to tt̄→W+bW -b̄, where both W
decay to quarks. We examine the top-antitop quark invariant
mass spectrum for the presence of narrow resonant states.
The search uses a data sample of pp̄ collisions at a center
of mass energy of 1.96 TeV collected by the CDF II detector
at the Fermilab Tevatron, with an integrated luminosity of
2.8fb-1. No evidence for top-antitop quark resonant
production is found. We place upper limits on the production
cross section times branching ratio for a specific topcolor
assisted technicolor model in which the Z′ has a width of
Γ Z′=0.012MZ′. Within this model, we exclude a Z′
boson with masses below 805GeV/c2 at the 95% confidence
level. © 2011 American Physical Society.},
Doi = {10.1103/PhysRevD.84.072003},
Key = {fds307871}
}
@article{fds307872,
Author = {Aaltonen, TEA},
Title = {Search for resonant production of $t\overline{t}$ pairs in
$4.8{\,}{\,}{\mathrm{fb}}^{\mathbf{-}1}$ of integrated
luminosity of $p\overline{p}$ collisions at
$\sqrt{s}\mathbf{=}1.96\text{\,}\text{\,}\mathrm{TeV}$},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {7},
Pages = {072004},
Publisher = {American Physical Society},
Year = {2011},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.84.072004},
Abstract = {We search for resonant production of tt̄ pairs in 4.8fb-1
integrated luminosity of pp̄ collision data at √s=1.96TeV
in the lepton+jets decay channel, where one top quark decays
leptonically and the other hadronically. A matrix-element
reconstruction technique is used; for each event a
probability density function of the tt̄ candidate invariant
mass is sampled. These probability density functions are
used to construct a likelihood function, whereby the cross
section for resonant tt̄ production is estimated, given a
hypothetical resonance mass and width. The data indicate no
evidence of resonant production of tt̄ pairs. A benchmark
model of leptophobic Z′→tt̄ is excluded with m
Z′<900GeV/c2 at 95% confidence level. © 2011 American
Physical Society.},
Doi = {10.1103/PhysRevD.84.072004},
Key = {fds307872}
}
@article{fds307665,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ},
Title = {Search for resonant top quark plus jet production in
tt̄+jets events with the ATLAS detector in pp collisions at
√s=7TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.86.091103},
Abstract = {This paper presents a search for a new heavy particle
produced in association with a top or antitop quark. Two
models in which the new heavy particle is a color singlet or
a color triplet are considered, decaying, respectively, to
t̄q or tq, leading to a resonance within the tt̄+jets
signature. The full 2011 ATLAS pp collision data set from
the LHC (4.7fb -1) is used to search for tt̄ events
produced in association with jets, in which one of the W
bosons from the top quarks decays leptonically and the other
decays hadronically. The data are consistent with the
Standard Model expectation, and a new particle with mass
below 430 Gev for both W ′ boson and color triplet models
is excluded at 95% confidence level, assuming unit
right-handed coupling. © 2012 CERN.},
Doi = {10.1103/PhysRevD.86.091103},
Key = {fds307665}
}
@article{fds307608,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and d'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro,
P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli,
F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu,
C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes,
L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Ranjan, N and Redondo Fernández and I and Renton, P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ,
J and Rusu, V and Safonov, A and Sakumoto, WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Sorin, V and Song, H and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner,
P and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson,
JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Search for resonant top-antitop production in the lepton
plus jets decay mode using the full CDF data
set.},
Journal = {Physical review letters},
Volume = {110},
Number = {12},
Pages = {121802},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.110.121802},
Abstract = {This Letter reports a search for a narrow resonant state
decaying into two W bosons and two b quarks where one W
boson decays leptonically and the other decays into a
quark-antiquark pair. The search is particularly sensitive
to top-antitop resonant production. We use the full data
sample of proton-antiproton collisions at a center-of-mass
energy of 1.96 TeV collected by the CDF II detector at the
Fermilab Tevatron, corresponding to an integrated luminosity
of 9.45 fb(-1). No evidence for resonant production is
found, and upper limits on the production cross section
times branching ratio for a narrow resonant state are
extracted. Within a specific benchmark model, we exclude a
Z' boson with mass, M(Z'), below 915 GeV/c(2) decaying into
a top-antitop pair at the 95% credibility level assuming a
Z' boson decay width of Γ(Z') = 0.012 M(Z'). This is the
most sensitive search for a narrow qq-initiated tt resonance
in the mass region below 750 GeV/c(2).},
Doi = {10.1103/physrevlett.110.121802},
Key = {fds307608}
}
@article{fds356632,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Search for resonant WZ production in the fully leptonic
final state in proton–proton collisions at s=13TeV with
the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {787},
Pages = {68-88},
Year = {2018},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2018.10.021},
Abstract = {A search for a heavy resonance decaying into WZ in the fully
leptonic channel (electrons and muons) is performed. It is
based on proton–proton collision data collected by the
ATLAS experiment at the Large Hadron Collider at a
centre-of-mass energy of 13 TeV, corresponding to an
integrated luminosity of 36.1 fb−1. No significant excess
is observed over the Standard Model predictions and limits
are set on the production cross section times branching
ratio of a heavy vector particle produced either in
quark–antiquark fusion or through vector-boson fusion.
Constraints are also obtained on the mass and couplings of a
singly charged Higgs boson, in the Georgi–Machacek model,
produced through vector-boson fusion.},
Doi = {10.1016/j.physletb.2018.10.021},
Key = {fds356632}
}
@article{fds372217,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios,
CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Albicocco,
P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire,
C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev,
V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Search for resonant WZ production in the fully leptonic
final state in proton–proton collisions at √s=13 TeV
with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11437-7},
Abstract = {A search for a WZ resonance, in the fully leptonic final
state (electrons or muons), is performed using 139 fb - 1
of data collected at a centre-of-mass energy of 13 TeV by
the ATLAS detector at the Large Hadron Collider. The results
are interpreted in terms of a singly charged Higgs boson of
the Georgi–Machacek model, produced by WZ fusion, and of a
Heavy Vector Triplet, with the resonance produced by WZ
fusion or the Drell–Yan process. No significant excess
over the Standard Model prediction is observed and limits
are set on the production cross-section times branching
ratio as a function of the resonance mass for these
processes.},
Doi = {10.1140/epjc/s10052-023-11437-7},
Key = {fds372217}
}
@article{fds310405,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Search for resonant WZ production in the WZ → ℓνℓ′
ℓ ′ channel in √ (s) = 7 TeV pp collisions with the
ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {June},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.85.112012},
Abstract = {A generic search is presented for a heavy particle decaying
to WZ → ℓν′ ℓ ′ (ℓ, ℓ′ = e, μ)final
states. The data were recorded by the ATLAS detector in
ffiffiffis √ s = 7 TeV pp collisions at the Large Hadron
Collider and correspond to an integrated luminosity of 1:02
fb-1. The transverse mass distribution of the selected WZ
candidates is found to be consistent with the standard model
expectation. Upper limits on the production cross section
times branching ratio are derived using two benchmark models
predicting a heavy particle decaying to a WZ
pair.},
Doi = {10.1103/PhysRevD.85.112012},
Key = {fds310405}
}
@article{fds310310,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
Title = {Search for s-channel single top-quark production in
proton-proton collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {740},
Pages = {118-136},
Publisher = {Elsevier BV},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2014.11.042},
Abstract = {This Letter presents a search at the LHC for s-channel
single top-quark production in proton-proton collisions at a
centre-of-mass energy of 8 TeV. The analyzed data set was
recorded by the ATLAS detector and corresponds to an
integrated luminosity of 20.3 fb-1. Selected events contain
one charged lepton, large missing transverse momentum and
exactly two b-tagged jets. A multivariate event classifier
based on boosted decision trees is developed to discriminate
s-channel single top-quark events from the main background
contributions. The signal extraction is based on a binned
maximum-likelihood fit of the output classifier
distribution. The analysis leads to an upper limit on the
s-channel single top-quark production cross-section of 14.6
pb at the 95% confidence level. The fit gives a
cross-section of σs = 5.0 ± 4.3 pb, consistent with the
Standard Model expectation.},
Doi = {10.1016/j.physletb.2014.11.042},
Key = {fds310310}
}
@article{fds307534,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández
Ramos, JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi, Y and Galloni, C and Garfinkel,
AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher,
C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee,
JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca,
G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane,
A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian,
C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan,
L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Vázquez, F and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao,
W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Search for s-channel single-top-quark production in events
with missing energy plus jets in pp collisions at sqrt[s] =
1.96 TeV.},
Journal = {Physical review letters},
Volume = {112},
Number = {23},
Pages = {231805},
Year = {2014},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.112.231805},
Abstract = {The first search for single-top-quark production from the
exchange of an s-channel virtual W boson using events with
an imbalance in the total transverse energy, b-tagged jets,
and no identified leptons is presented. Assuming the
electroweak production of top quarks of mass 172.5 GeV/c(2)
in the s channel, a cross section of 1.12(-0.57)(+0.61)
(stat+syst) pb with a significance of 1.9 standard
deviations is measured. This measurement is combined with
the result obtained from events with an imbalance in total
transverse momentum, b-tagged jets, and exactly one
identified lepton, yielding a cross section of
1.36(-0.32)(+0.37) (stat+syst) pb, with a significance of
4.2 standard deviations.},
Doi = {10.1103/physrevlett.112.231805},
Key = {fds307534}
}
@article{fds307773,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonak, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Search for same-sign top-quark production and
fourth-generation down-type quarks in pp collisions at √s
= 7 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {4},
Publisher = {Springer Nature},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2012)069},
Abstract = {A search is presented for same-sign top-quark production and
down-type heavy quarks of charge -1/3 in events with two
isolated leptons (e or μ) that have the same electric
charge, at least two jets and large missing transverse
momentum. The data are selected from pp collisions at ps = 7
TeV recorded by the ATLAS detector and correspond to an
integrated luminosity of 1.04 fb-1. The observed data are
consistent with expectations from Standard Model processes.
Upper limits are set at 95% confidence level on the cross
section of new sources of same-sign top-quark pair
production of 1.4-2.0 pb depending on the assumed mediator
mass. Upper limits are also set on the pair-production
cross-section for new heavy down-type quarks; a lower limit
of 450 GeV is set at 95% confidence level on the mass of
heavy down-type quarks under the assumption that they decay
100% of the time to Wt. Copyright CERN.},
Doi = {10.1007/JHEP04(2012)069},
Key = {fds307773}
}
@article{fds307706,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati,
S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard,
R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli,
F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji,
W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi,
M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B},
Title = {Search for scalar bottom quark pair production with the
ATLAS detector in pp collisions at sqrt[s]=7 TeV.},
Journal = {Physical review letters},
Volume = {108},
Number = {18},
Pages = {181802},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.108.181802},
Abstract = {The results of a search for pair production of the scalar
partners of bottom quarks in 2.05 fb(-1) of pp
collisions at sqrt[s]=7 TeV using the ATLAS experiment
are reported. Scalar bottom quarks are searched for in
events with large missing transverse momentum and two jets
in the final state, where both jets are identified as
originating from a bottom quark. In an R-parity conserving
minimal supersymmetric scenario, assuming that the scalar
bottom quark decays exclusively into a bottom quark and a
neutralino, 95% confidence-level upper limits are obtained
in the b(1) - χ(1)(0) mass plane such that for neutralino
masses below 60 GeV scalar bottom masses up to 390 GeV are
excluded.},
Doi = {10.1103/physrevlett.108.181802},
Key = {fds307706}
}
@article{fds310288,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek,
T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boddy, CR and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm,
C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde,
A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill,
R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow,
BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Ciocio, A and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta, C},
Title = {Search for Scalar Charm Quark Pair Production in pp
Collisions at sqrt[s]=8 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {114},
Number = {16},
Pages = {161801},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.114.161801},
Abstract = {The results of a dedicated search for pair production of
scalar partners of charm quarks are reported. The search is
based on an integrated luminosity of 20.3 fb^{-1} of pp
collisions at sqrt[s]=8 TeV recorded with the ATLAS
detector at the LHC. The search is performed using events
with large missing transverse momentum and at least two
jets, where the two leading jets are each tagged as
originating from c quarks. Events containing isolated
electrons or muons are vetoed. In an R-parity-conserving
minimal supersymmetric scenario in which a single
scalar-charm state is kinematically accessible, and where it
decays exclusively into a charm quark and a neutralino, 95%
confidence-level upper limits are obtained in the
scalar-charm-neutralino mass plane such that, for neutralino
masses below 200 GeV, scalar-charm masses up to 490 GeV
are excluded.},
Doi = {10.1103/physrevlett.114.161801},
Key = {fds310288}
}
@article{fds310350,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Akesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Asman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Search for scalar diphoton resonances in the mass range
65-600 GeV with the ATLAS detector in pp collision data at
√s=8 TeV.},
Journal = {Physical review letters},
Volume = {113},
Number = {17},
Pages = {171801},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1103/physrevlett.113.171801},
Abstract = {A search for scalar particles decaying via narrow resonances
into two photons in the mass range 65-600 GeV is performed
using 20.3 fb(-1) of √s 8 TeV pp collision data
collected with the ATLAS detector at the Large Hadron
Collider. The recently discovered Higgs boson is treated as
a background. No significant evidence for an additional
signal is observed. The results are presented as limits at
the 95% confidence level on the production cross section of
a scalar boson times branching ratio into two photons, in a
fiducial volume where the reconstruction efficiency is
approximately independent of the event topology. The upper
limits set extend over a considerably wider mass range than
previous searches.},
Doi = {10.1103/physrevlett.113.171801},
Key = {fds310350}
}
@booklet{Abbott97a,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G and Fisk, HE and Fisyak, Y and Flattum, E},
Title = {Search for scalar leptoquark pairs decaying to electrons and
jets in p®p collisions},
Journal = {Physical Review Letters},
Volume = {79},
Number = {22},
Pages = {4321-4326},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.79.4321},
Abstract = {We have searched for the pair production of first generation
scalar leptoquarks in the eejj channel using the full data
set (123pb−1) collected with the D0 detector at the
Fermilab Tevatron during 1992-1996. We observe no candidates
with an expected background of approximately 0.4 events.
Comparing the experimental 95% confidence level upper limit
to theoretical calculations of the cross section with the
assumption of a 100% branching fraction of eq, we set a
lower limit on the mass of a first generation scalar
leptoquark of 225 GeV/c2. The results of this analysis rule
out the interpretation of the excess of high Q2 events at
DESY HERA as leptoquarks which decay exclusively to eq. ©
1997 The American Physical Society.},
Doi = {10.1103/PhysRevLett.79.4321},
Key = {Abbott97a}
}
@article{fds308155,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Belloni, A and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Bortoletto, D and Boudreau, J and Bourov, S and Bromberg, C and Brubaker, E and Budagov,
J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell, M and Canelli, F and Canepa,
A and Casarsa, M and Carlsmith, D and Carron, S and Carosi, R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri,
A and Cerrito, L and Chapman, J and Chen, YC and Chertok, M and Chiarelli,
G and Chlachidze, G and Chlebana, F and Cho, I and Cho, K and Chokheli, D and Chou, JP and Chuang, S and Chung, K and Chung, WH and Chung, YS and Cijliak, M and Ciobanu, CI and Ciocci, MA and Clark, AG and Clark, D and Coca, M and Connolly, A and Convery, M and Conway,
J},
Title = {Search for scalar leptoquark pairs decaying to νν̄qq̄ in
pp̄ collisions at s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {11},
Pages = {1-7},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.71.112001},
Abstract = {We report on a search for the pair production of scalar
leptoquarks (LQ), using 191pb-1 of proton-antiproton
collision data recorded by the CDF experiment during Run II
of the Tevatron. The leptoquarks are sought via their decay
into a neutrino and quark yielding missing transverse energy
and several jets of large transverse energy. No evidence for
LQ production is observed, and limits are set on
σ(pp̄→LQLQ̄X→νν̄qq̄X). Using a next-to-leading
order theoretical prediction of the cross section for LQ
production, we exclude first-generation LQ in the mass
interval 78 to 117GeV/c2 at the 95% confidence level for
BR(LQ→νq)=100%. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevD.71.112001},
Key = {fds308155}
}
@article{fds321090,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen,
G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders,
CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for scalar leptoquarks in pp collisions at √S =
13TeV with the ATLAS experiment},
Journal = {New Journal of Physics},
Volume = {18},
Number = {9},
Pages = {1-25},
Publisher = {IOP Publishing},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1088/1367-2630/18/9/093016},
Abstract = {An inclusive search for a new-physics signature of
lepton-jet resonances has been performed by the ATLAS
experiment. Scalar leptoquarks, pair-produced in pp
collisions at s √S13 TeV at the large hadron collider,
have been considered. An integrated luminosity of 3.2
fb−1, corresponding to the full 2015 dataset was used.
First (second) generation leptoquarks were sought in events
with two electrons (muons) and two or more jets. The
observed event yield in each channel is consistent with
Standard Model background expectations. The observed
(expected) lower limits on the leptoquark mass at 95%
confidence level are 1100 and 1050 GeV (1160 and 1040 GeV)
for first and second generation leptoquarks, respectively,
assuming a branching ratio into a charged lepton and a quark
of 100%. Upper limits on the aforementioned branching ratio
are also given as a function of leptoquark mass. Compared
with the results of earlier ATLAS searches, the sensitivity
is increased for leptoquark masses above 860 GeV, and the
observed exclusion limits confirm and extend the published
results.},
Doi = {10.1088/1367-2630/18/9/093016},
Key = {fds321090}
}
@article{fds356588,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA},
Title = {Search for scalar resonances decaying into μ +
μ − in events with and without b-tagged jets
produced in proton-proton collisions at √s=13 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {7},
Year = {2019},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2019)117},
Abstract = {A search for a narrow scalar resonance decaying into an
opposite-sign muon pair produced in events with and without
b-tagged jets is presented in this paper. The search uses
36.1 fb−1 of s=13 TeV proton-proton collision data
recorded by the ATLAS experiment at the LHC. No significant
excess of events above the expected Standard Model
background is observed in the investigated mass range of 0.2
to 1.0 TeV. The observed upper limits at 95% confidence
level on the cross section times branching ratio for b-quark
associated production and gluon-gluon fusion are between 1.9
and 41 fb and 1.6 and 44 fb respectively, which is
consistent with expectations.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP07(2019)117},
Key = {fds356588}
}
@article{fds307791,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós,
G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber,
T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth,
CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom,
PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni,
G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini,
G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
J and Colon, G and Muiño, PC and Coniavitis, E and Conidi,
MC},
Title = {Search for scalar top quark pair production in natural gauge
mediated supersymmetry models with the ATLAS detector in pp
collisions at s=7TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {715},
Number = {1-3},
Pages = {44-60},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.07.010},
Abstract = {The results of a search for pair production of the lighter
scalar partners of top quarks (t~1) in 2.05 fb-1 of pp
collisions at s=7 TeV using the ATLAS experiment at the LHC
are reported. Scalar top quarks are searched for in events
with two same flavour opposite-sign leptons (e, μ) with
invariant mass consistent with the Z boson mass, large
missing transverse momentum and jets in the final state. At
least one of the jets is identified as originating from a
b-quark. No excess over Standard Model expectations is
found. The results are interpreted in the framework of
R-parity conserving, gauge mediated Supersymmetry breaking
'natural' scenarios, where the neutralino (χ~10) is the
next-to-lightest supersymmetric particle. Scalar top quark
masses up to 310 GeV are excluded for 115GeV<mχ~10<230GeV
at 95% confidence level, reaching an exclusion of
mt~1<330GeV for mχ~10=190GeV. Scalar top quark masses
below 240 GeV are excluded for all values of mχ~10>mZ.
© 2012 CERN.},
Doi = {10.1016/j.physletb.2012.07.010},
Key = {fds307791}
}
@article{fds310402,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d’Ascenzo, N and Datta, M and de
Barbaro, P and Dell’Orso, M and Demortier, L and Deninno, M and Devoto, F and d’Errico, M},
Title = {Search for scalar top quark production in (Formula
presented.) collisions at (Formula presented.) = 1.96
TeV},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {10},
Publisher = {Springer Nature},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2012)158},
Abstract = {We report on a search for the supersymmetric partner of the
top quark (scalar top) decaying into a charm quark and a
neutralino in (Formula presented.) collisions at (Formula
presented.) = 1.96TeV. The data sample, collected by the CDF
II detector at the Fermilab Tevatron, corresponds to an
integrated luminosity of 2.6 fb<sup>−1</sup>. Candidate
events are selected by requiring two or more jets and a
large imbalance in the transverse momentum. To enhance the
analysis sensitivity, at least one of the jets is required
to be identified as originating from a charm quark using an
algorithm specifically designed for this analysis. The
selected events are in good agreement with standard model
predictions. In the case of large mass splitting between the
scalar top quark and the neutralino we exclude a scalar top
quark mass below 180 GeV/c<sup>2</sup> at 95% confidence
level.},
Doi = {10.1007/JHEP10(2012)158},
Key = {fds310402}
}
@article{fds308218,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Bross, A and Buchholz, D and Burtovoi,
VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros, Y and Dudko,
LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher,
S and Fein, D and Ferbel, T and Fisk, HE and Fisyak,
Y},
Title = {Search for second generation leptoquark pairs decaying to
μv + jets in pp collisons at √ s = 1.8
Tev},
Journal = {Physical Review Letters},
Volume = {83},
Number = {15},
Pages = {2896-2901},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.83.2896},
Abstract = {We report on a search for second generation leptoquarks (LQ)
produced in pp collisions at √ = 1.8TeV using the D0
detector at Fermilab. Second generation leptoquarks are
assumed to be produced in pairs and to decay to either μ or
v and either a strange or a charm quark (q). Limits are
placed on σ (pp → LQLQ → μ v + jets) as a function of
the mass of the leptoquark. For equal branching ratios to
μq and vq second generation scalar leptoquarks with a mass
below 160 GeV/c2 vector leptoquarks with anomalous minimal
vector couplings with a mass below 240 GeV/c2 and vector
leptoquarks with Yang-Mills couplings with a mass below 290
GeV/c2 are excluded at the 95% confidence level. © 1999 The
American Physical Society.},
Doi = {10.1103/PhysRevLett.83.2896},
Key = {fds308218}
}
@article{fds307781,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Search for second generation scalar leptoquarks in pp
collisions at √s = 7 TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {9},
Pages = {1-21},
Publisher = {Springer Nature},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2151-6},
Abstract = {The results of a search for the production of second
generation scalar leptoquarks are presented for final states
consisting of either two muons and at least two jets or a
muon plus missing transverse momentum and at least two jets.
A total of 1.03 fb<sup>−1</sup> integrated luminosity of
protonproton collision data produced by the Large Hadron
Collider at √s = 7 TeV and recorded by the ATLAS detector
is used for the search. The event yields in the signal
regions are found to be consistent with the Standard Model
background expectations. The production of second generation
leptoquarks is excluded for a leptoquark mass m<inf>LQ</inf>
< 594 (685) GeV at 95 % confidence level, for a branching
ratio of 0.5 (1.0) for leptoquark decay to a muon and a
quark.},
Doi = {10.1140/epjc/s10052-012-2151-6},
Key = {fds307781}
}
@article{fds332358,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Burtovoi,
VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison,
J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
T and Fatyga, MK and Feher, S and Fein, D and Ferbel,
T},
Title = {Search for second-generation leptoquark pairs in ¯pp
collisions at √s=1.8TeV},
Journal = {Physical Review Letters},
Volume = {84},
Number = {10},
Pages = {2088-2093},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.2088},
Abstract = {We have searched for second-generation leptoquark (LQ) pairs
in the μμ+jets channel using 94 ±5pb−1 of ¯pp collider
data collected by the D0 experiment at the Fermilab Tevatron
during 1993–1996. No evidence for a signal is observed.
These results are combined with those from the μν+jets and
νν+jets channels to obtain 95% confidence level (C.L.)
upper limits on the LQ pair production cross section as a
function of mass and β, the branching fraction of a LQ
decay into a charged lepton and a quark. Lower limits of
200(180)GeV/c2 for β=1(1/2) are set at the 95% C.L. on the
mass of scalar LQ. Mass limits are also set on vector
leptoquarks as a function of β. © 2000 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.84.2088},
Key = {fds332358}
}
@article{fds308150,
Author = {Abulencia, and A, and others},
Title = {Search for second-generation scalar leptoquarks in
$p\bar{p}$ collisions at $\sqrt{s} =$ 1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {5},
Pages = {051102},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.72.051107},
Abstract = {Results on a search for pair production of second generation
scalar leptoquark in p anti-p collisions at s**(1/2) = 1.96
TeV are reported. The data analyzed were collected by the
CDF detector during the 2002-2003 Tevatron Run II and
correspond to an integrated luminosity of 198 pb-1.
Leptoquarks (LQ) are sought through their decay into
(charged) leptons and quarks, with final state signatures
represented by two muons and jets and one muon, large
transverse missing energy and jets. We observe no evidence
for LQ production and derive 95% C.L. upper limits on the LQ
production cross sections as well as lower limits on their
mass as a function of Beta, where Beta is the branching
fraction for LQ --> mu q.},
Doi = {10.1103/PhysRevD.72.051107},
Key = {fds308150}
}
@article{fds356789,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Ochoa, MI and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S},
Title = {Search for single b⁎-quark production with the
ATLAS detector at √s=7 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {721},
Number = {4-5},
Pages = {171-189},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2013.03.016},
Abstract = {The results of a search for an excited bottom-quark b⁎ in
pp collisions at s=7 TeV, using 4.7 fb−1 of data collected
by the ATLAS detector at the LHC are presented. In the model
studied, a single b⁎-quark is produced through a
chromomagnetic interaction and subsequently decays to a W
boson and a top quark. The search is performed in the
dilepton and lepton + jets final states, which are combined
to set limits on b⁎-quark couplings for a range of
b⁎-quark masses. For a benchmark with unit size
chromomagnetic and Standard Model-like electroweak b⁎
couplings, b⁎ quarks with masses less than 870 GeV are
excluded at the 95% credibility level.},
Doi = {10.1016/j.physletb.2013.03.016},
Key = {fds356789}
}
@article{fds315924,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O},
Title = {Search for single production of a vector-like quark via a
heavy gluon in the 4b final state with the ATLAS detector in
pp collisions at s=8 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {758},
Pages = {249-268},
Publisher = {Elsevier BV},
Year = {2016},
Month = {July},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2016.04.061},
Abstract = {A search is performed for the process pp→G*→BHb-/B-Hb→Hbb-→bb-bb-,
predicted in composite Higgs scenarios, where G* is a heavy
colour octet vector resonance and BH a vector-like quark of
charge -1/3. The data were obtained from pp collisions at a
centre-of-mass energy of 8 TeV corresponding to an
integrated luminosity of 19.5 fb-1, recorded by the ATLAS
detector at the LHC. The largest background, multijet
production, is estimated using a data-driven method. No
significant excess of events with respect to Standard Model
predictions is observed, and upper limits on the production
cross section times branching ratio are set. Comparisons to
the predictions from a specific benchmark model are made,
resulting in lower mass limits in the two-dimensional mass
plane of mG* vs. mBH.},
Doi = {10.1016/j.physletb.2016.04.061},
Key = {fds315924}
}
@article{fds321106,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
LB and Barreiro, F and Costa, JBGD and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella,
G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and de
Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni,
G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, YL and Chang, P and Chapman, JD and Charlton,
DG and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Colasurdo, L and Cole, B and Cole, S and Colijn, AP and Collot, J and Colombo, T and Compostella,
G},
Title = {Search for single production of vector-like quarks decaying
into Wb in pp collisions at [Formula: see
text] TeV with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {8},
Pages = {442},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4281-8},
Abstract = {A search for singly produced vector-like <i>Q</i> quarks,
where <i>Q</i> can be either a <i>T</i> quark with charge
[Formula: see text] or a <i>Y</i> quark with charge
[Formula: see text], is performed in proton-proton
collisions recorded with the ATLAS detector at the LHC. The
dataset corresponds to an integrated luminosity of 20.3
fb[Formula: see text] and was produced with a centre-of-mass
energy of [Formula: see text] TeV. This analysis targets
[Formula: see text] decays where the <i>W</i> boson decays
leptonically. A veto on massive large-radius jets is used to
reject the dominant [Formula: see text] background. The
reconstructed <i>Q</i>-candidate mass, ranging from 0.4 to
1.2 TeV, is used in the search to discriminate signal from
background processes. No significant deviation from the
Standard Model expectation is observed, and limits are set
on the [Formula: see text] cross-section times branching
ratio. The results are also interpreted as limits on the
<i>QWb</i> coupling and the mixing with the Standard Model
sector for a singlet <i>T</i> quark or a <i>Y</i> quark from
a doublet. <i>T</i> quarks with masses below 0.95 TeV are
excluded at 95 % confidence level, assuming a unit coupling
and a BR[Formula: see text], whereas the expected limit is
1.10 TeV.},
Doi = {10.1140/epjc/s10052-016-4281-8},
Key = {fds321106}
}
@article{fds356605,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Search for single production of vector-like quarks decaying
into Wb in pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2019)164},
Abstract = {A search for singly produced vector-like quarks Q, where Q
can be either a T quark with charge +2/3 or a Y quark with
charge −4/3, is performed in proton–proton collision
data at a centre-of-mass energy of 13 TeV corresponding to
an integrated luminosity of 36.1 fb−1, recorded with the
ATLAS detector at the LHC in 2015 and 2016. The analysis
targets Q → Wb decays where the W boson decays
leptonically. No significant deviation from the expected
Standard Model background is observed. Upper limits are set
on the QWb coupling strength and the mixing between the
Standard Model sector and a singlet T quark or a Y quark
from a (B, Y) doublet or a (T, B, Y) triplet, taking into
account the interference effects with the Standard Model
background. The upper limits set on the mixing angle are as
small as |sin θL| = 0.18 for a singlet T quark of mass 800
GeV, |sin θR| = 0.17 for a Y quark of mass 800 GeV in a (B,
Y) doublet model and |sin θL| = 0.16 for a Y quark of mass
800 GeV in a (T, B, Y) triplet model. Within a (B, Y)
doublet model, the limits set on the mixing parameter |sin
θR| are comparable with the exclusion limits from
electroweak precision observables in the mass range between
about 900 GeV and 1250 GeV.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP05(2019)164},
Key = {fds356605}
}
@article{fds308185,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Boos, EE and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler,
JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del
Signore, K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and di Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Duensing,
S},
Title = {Search for single top quark production at DØ using neural
networks},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {517},
Number = {3-4},
Pages = {282-294},
Publisher = {Elsevier BV},
Year = {2001},
Month = {October},
url = {http://dx.doi.org/10.1016/S0370-2693(01)01009-7},
Abstract = {We present a search for electroweak production of single top
quarks in ≈90 pb-1 of data collected with the DØ detector
at the Fermilab Tevatron collider. Using arrays of neural
networks to separate signals from backgrounds, we set upper
limits on the cross sections of 17 pb for the s-channel
process pp̄ → tb + X, and 22 pb for the t-channel process
pp̄ → tqb + X, both at the 95% confidence level. © 2001
Elsevier Science B.V. All rights reserved.},
Doi = {10.1016/S0370-2693(01)01009-7},
Key = {fds308185}
}
@article{fds307918,
Author = {Aaltonen, and T, and others},
Title = {Search for single top quark production in $\bar{p} p$
collisions at $\sqrt{s} = 1.96$ TeV in the missing
transverse energy plus jets topology},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.072003},
Abstract = {http://arxiv.org/abs/1001.4577},
Doi = {10.1103/PhysRevD.81.072003},
Key = {fds307918}
}
@article{fds308222,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Alves, GA and Amos, N and Anderson,
EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland,
T and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Search for squarks and gluinos in events containing jets and
a large imbalance in transverse energy},
Journal = {Physical Review Letters},
Volume = {83},
Number = {24},
Pages = {4937-4942},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.83.4937},
Abstract = {Using data corresponding to an integrated luminosity of
79pb−1, D0 has searched for events containing multiple
jets and large missing transverse energy in pp¯ collisions
at √s = 1.8TeV at the Fermilab Tevatron collider.
Observing no significant excess beyond what is expected from
the standard model, we set limits on the masses of squarks
and gluinos and on the model parameters m0 and m1/2, in the
framework of the minimal low-energy supergravity models of
supersymmetry. For tanβ=2 and A0 = 0, with μ < 0, we
exclude all models with m˜q<250 GeV/c2. For models with
equal squark and gluino masses, we exclude m < 260 GeV/c2.
© 1999 The American Physical Society.},
Doi = {10.1103/PhysRevLett.83.4937},
Key = {fds308222}
}
@article{fds356720,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Search for squarks and gluinos in events with an isolated
lepton, jets, and missing transverse momentum at √s=13 TeV
with the ATLAS detector},
Journal = {Physical Review D},
Volume = {96},
Number = {11},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevD.96.112010},
Abstract = {The results of a search for squarks and gluinos in final
states with an isolated electron or muon, multiple jets and
large missing transverse momentum using proton-proton
collision data at a center-of-mass energy of √ = 13 TeV
are presented. The data set used was recorded during 2015
and 2016 by the ATLAS experiment at the Large Hadron
Collider and corresponds to an integrated luminosity of 36.1
fb-1. No significant excess beyond the expected background
is found. Exclusion limits at 95% confidence level are set
in a number of supersymmetric scenarios, reaching masses up
to 2.1 TeV for gluino pair production and up to 1.25 TeV for
squark pair production.},
Doi = {10.1103/PhysRevD.96.112010},
Key = {fds356720}
}
@article{fds346229,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M},
Title = {Search for squarks and gluinos in events with hadronically
decaying tau leptons, jets and missing transverse momentum
in proton-proton collisions at [Formula: see text] TeV
recorded with the ATLAS detector.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {12},
Pages = {683},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4481-2},
Abstract = {A search for supersymmetry in events with large missing
transverse momentum, jets, and at least one hadronically
decaying tau lepton has been performed using
3.2 fb[Formula: see text] of proton-proton collision data
at [Formula: see text] recorded by the ATLAS detector at the
Large Hadron Collider in 2015. Two exclusive final states
are considered, with either exactly one or at least two tau
leptons. No excess over the Standard Model prediction is
observed in the data. Results are interpreted in the context
of gauge-mediated supersymmetry breaking and a simplified
model of gluino pair production with tau-rich cascade
decays, substantially improving on previous limits. In the
GMSB model considered, supersymmetry-breaking scale
([Formula: see text]) values below [Formula: see text] are
excluded at the 95% confidence level, corresponding to
gluino masses below [Formula: see text]. For large values of
[Formula: see text], values of [Formula: see text] up to
[Formula: see text] and gluino masses up to [Formula: see
text] are excluded. In the simplified model, gluino masses
are excluded up to [Formula: see text] for neutralino masses
around [Formula: see text]. Neutralino masses below
[Formula: see text] are excluded for all gluino masses
between 800 and [Formula: see text], while the strongest
exclusion of [Formula: see text] is achieved for gluino
masses around [Formula: see text].},
Doi = {10.1140/epjc/s10052-016-4481-2},
Key = {fds346229}
}
@article{fds310292,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia,
M},
Title = {Search for squarks and gluinos in events with isolated
leptons, jets and missing transverse momentum at √s = 8
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {4},
Publisher = {Springer Nature},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2015)116},
Abstract = {The results of a search for supersymmetry in final states
containing at least one isolated lepton (electron or muon),
jets and large missing transverse momentum with the ATLAS
detector at the Large Hadron Collider are reported. The
search is based on proton-proton collision data at a
centre-of-mass energy √ = 8 TeV collected in 2012,
corresponding to an integrated luminosity of 20 fb−1. No
significant excess above the Standard Model expectation is
observed. Limits are set on supersymmetric particle masses
for various supersymmetric models. Depending on the model,
the search excludes gluino masses up to 1.32 TeV and squark
masses up to 840 GeV. Limits are also set on the parameters
of a minimal universal extra dimension model, excluding a
compactification radius of 1/Rc = 950 GeV for a cut-off
scale times radius (ΛRc) of approximately
30.},
Doi = {10.1007/JHEP04(2015)116},
Key = {fds310292}
}
@article{fds347452,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O},
Title = {Search for squarks and gluinos in final states with
hadronically decaying τ -leptons, jets, and missing
transverse momentum using pp collisions at s =13 TeV with
the ATLAS detector},
Journal = {Physical Review D},
Volume = {99},
Number = {1},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.99.012009},
Abstract = {A search for supersymmetry in events with large missing
transverse momentum, jets, and at least one hadronically
decaying τ-lepton is presented. Two exclusive final states
with either exactly one or at least two τ-leptons are
considered. The analysis is based on proton-proton
collisions at s=13 TeV corresponding to an integrated
luminosity of 36.1 fb-1 delivered by the Large Hadron
Collider and recorded by the ATLAS detector in 2015 and
2016. No significant excess is observed over the Standard
Model expectation. At 95% confidence level,
model-independent upper limits on the cross section are set
and exclusion limits are provided for two signal scenarios:
a simplified model of gluino pair production with τ-rich
cascade decays, and a model with gauge-mediated
supersymmetry breaking (GMSB). In the simplified model,
gluino masses up to 2000 GeV are excluded for low values of
the mass of the lightest supersymmetric particle (LSP),
while LSP masses up to 1000 GeV are excluded for gluino
masses around 1400 GeV. In the GMSB model, values of the
supersymmetry-breaking scale are excluded below 110 TeV for
all values of tanβ in the range 2≤tanβ≤60, and below
120 TeV for tanβ>30.},
Doi = {10.1103/PhysRevD.99.012009},
Key = {fds347452}
}
@article{fds321117,
Author = {Atlas Collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas
Kuutmann, E and Berger, N and Beringer, J and Berlendis, S and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd,
J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton, D and Britzger, D and Brochu,
FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks,
WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro,
R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {Search for squarks and gluinos in final states with jets and
missing transverse momentum at [Formula: see text] =13
[Formula: see text]with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {7},
Pages = {392},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4184-8},
Abstract = {A search for squarks and gluinos in final states containing
hadronic jets, missing transverse momentum but no electrons
or muons is presented. The data were recorded in 2015 by the
ATLAS experiment in [Formula: see text] proton-proton
collisions at the Large Hadron Collider. No excess above the
Standard Model background expectation was observed in
3.2 [Formula: see text] of analyzed data. Results are
interpreted within simplified models that assume
<i>R</i>-parity is conserved and the neutralino is the
lightest supersymmetric particle. An exclusion limit at the
95 % confidence level on the mass of the gluino is set at
1.51 [Formula: see text] for a simplified model
incorporating only a gluino octet and the lightest
neutralino, assuming the lightest neutralino is massless.
For a simplified model involving the strong production of
mass-degenerate first- and second-generation squarks, squark
masses below 1.03 [Formula: see text] are excluded for a
massless lightest neutralino. These limits substantially
extend the region of supersymmetric parameter space excluded
by previous measurements with the ATLAS detector.},
Doi = {10.1140/epjc/s10052-016-4184-8},
Key = {fds321117}
}
@article{fds355441,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for squarks and gluinos in final states with jets and
missing transverse momentum using 139 fb −1 of
√s = 13 TeV pp collision data with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {2},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2021)143},
Abstract = {A search for the supersymmetric partners of quarks and
gluons (squarks and gluinos) in final states containing jets
and missing transverse momentum, but no electrons or muons,
is presented. The data used in this search were recorded by
the ATLAS experiment in proton-proton collisions at a
centre-of-mass energy of s = 13 TeV during Run 2 of the
Large Hadron Collider, corresponding to an integrated
luminosity of 139 fb−1. The results are interpreted in the
context of various R-parity-conserving models where squarks
and gluinos are produced in pairs or in association and a
neutralino is the lightest supersymmetric particle. An
exclusion limit at the 95% confidence level on the mass of
the gluino is set at 2.30 TeV for a simplified model
containing only a gluino and the lightest neutralino,
assuming the latter is massless. For a simplified model
involving the strong production of mass-degenerate first-
and second-generation squarks, squark masses below 1.85 TeV
are excluded if the lightest neutralino is massless. These
limits extend substantially beyond the region of
supersymmetric parameter space excluded previously by
similar searches with the ATLAS detector. [Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP02(2021)143},
Key = {fds355441}
}
@article{fds356680,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Search for squarks and gluinos in final states with jets and
missing transverse momentum using 36 fb-1 of √s =13 TeV pp
collision data with the ATLAS detector},
Journal = {Physical Review D},
Volume = {97},
Number = {11},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.97.112001},
Abstract = {A search for the supersymmetric partners of quarks and
gluons (squarks and gluinos) in final states containing
hadronic jets and missing transverse momentum, but no
electrons or muons, is presented. The data used in this
search were recorded in 2015 and 2016 by the ATLAS
experiment in s=13 TeV proton-proton collisions at the Large
Hadron Collider, corresponding to an integrated luminosity
of 36.1 fb-1. The results are interpreted in the context of
various models where squarks and gluinos are pair produced
and the neutralino is the lightest supersymmetric particle.
An exclusion limit at the 95% confidence level on the mass
of the gluino is set at 2.03 TeV for a simplified model
incorporating only a gluino and the lightest neutralino,
assuming the lightest neutralino is massless. For a
simplified model involving the strong production of
mass-degenerate first- and second-generation squarks, squark
masses below 1.55 TeV are excluded if the lightest
neutralino is massless. These limits substantially extend
the region of supersymmetric parameter space previously
excluded by searches with the ATLAS detector.},
Doi = {10.1103/PhysRevD.97.112001},
Key = {fds356680}
}
@article{fds366275,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for squarks and gluinos in final states with one
isolated lepton, jets, and missing transverse momentum at
√s=13 with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09344-w},
Abstract = {The results of a search for gluino and squark pair
production with the pairs decaying via the lightest
charginos into a final state consisting of two W bosons, the
lightest neutralinos (χ~10), and quarks, are presented: the
signal is characterised by the presence of a single charged
lepton (e± or μ±) from a W boson decay, jets, and missing
transverse momentum. The analysis is performed using
139 fb- 1 of proton–proton collision data taken at a
centre-of-mass energy s=13 delivered by the Large Hadron
Collider and recorded by the ATLAS experiment. No
statistically significant excess of events above the
Standard Model expectation is found. Limits are set on the
direct production of squarks and gluinos in simplified
models. Masses of gluino (squark) up to 2.2 (1.4) are
excluded at 95% confidence level for a light
χ~10.},
Doi = {10.1140/epjc/s10052-021-09344-w},
Key = {fds366275}
}
@article{fds350334,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V},
Title = {Search for squarks and gluinos in final states with
same-sign leptons and jets using 139 fb −1 of
data collected with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {6},
Year = {2020},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2020)046},
Abstract = {A search for supersymmetric partners of gluons and quarks is
presented, involving signatures with jets and either two
isolated leptons (electrons or muons) with the same electric
charge, or at least three isolated leptons. A data sample of
proton-proton collisions at s = 13 TeV recorded with the
ATLAS detector at the Large Hadron Collider between 2015 and
2018, corresponding to a total integrated luminosity of 139
fb−1, is used for the search. No significant excess over
the Standard Model expectation is observed. The results are
interpreted in simplified supersymmetric models featuring
both R-parity conservation and R-parity violation, raising
the exclusion limits beyond those of previous ATLAS searches
to 1600 GeV for gluino masses and 750 GeV for bottom and top
squark masses in these scenarios. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP06(2020)046},
Key = {fds350334}
}
@article{fds308212,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G},
Title = {Search for squarks and gluinos in single-photon events with
jets and large missing transverse energy in p¯p collisions
at √ s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {82},
Number = {1},
Pages = {29-34},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.29},
Abstract = {We search for new physics using events with one high
transverse energy photon, two or more jets, and an apparent
imbalance in transverse energy, in pp¯ collisions at the
Fermilab Tevatron at √ s=1.8TeV. Such events are predicted
for production of supersymmetric particles in some models.
No excess is observed beyond expected background. For the
parameter space of the minimal supersymmetric standard model
with branching fraction B(∼ Χ02→ = γ ∼ Χ01) = 1 and
mΧ02- mΧ01> 20 GeV, we obtain a 95% confidence level lower
mass limit of 310 GeV for equal mass squarks and gluinos.
The results are also interpreted in models with low energy
gauge mediated supersymmetry breaking. © 1999 The American
Physical Society.},
Doi = {10.1103/PhysRevLett.82.29},
Key = {fds308212}
}
@article{fds307755,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Search for squarks and gluinos using final states with jets
and missing transverse momentum with the Atlas detector in
s=7 TeV proton-proton collisions},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {710},
Number = {1},
Pages = {67-85},
Publisher = {Elsevier BV},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2012.02.051},
Abstract = {A search for squarks and gluinos in events containing jets,
missing transverse momentum and no electrons or muons is
presented. The data were recorded in 2011 by the ATLAS
experiment in s=7 TeV proton-proton collisions at the Large
Hadron Collider. No excess above the Standard Model
background expectation is observed in 1.04 fb-1 of data.
Gluino and squark masses below 700 GeV and 875 GeV
respectively are excluded at the 95% confidence level in
simplified models containing only squarks of the first two
generations, a gluino octet and a massless neutralino. The
exclusion limit increases to 1075 GeV for squarks and
gluinos of equal mass. In MSUGRA/CMSSM models with tanβ=10,
A0=0 and μ>0, squarks and gluinos of equal mass are
excluded for masses below 950 GeV. These limits extend the
region of supersymmetric parameter space excluded by
previous measurements. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.02.051},
Key = {fds307755}
}
@article{fds307633,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for squarks and gluinos with the ATLAS detector in
final states with jets and missing transverse momentum using
4.7 fb-1 of √s=7 TeV proton-proton collision
data},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.87.012008},
Abstract = {A search for squarks and gluinos in final states containing
jets, missing transverse momentum and no high-pT electrons
or muons is presented. The data represent the complete
sample recorded in 2011 by the ATLAS experiment in 7 TeV
proton-proton collisions at the Large Hadron Collider, with
a total integrated luminosity of 4.7 fb-1. No excess above
the Standard Model background expectation is observed.
Gluino masses below 860 GeV and squark masses below 1320 GeV
are excluded at the 95% confidence level in simplified
models containing only squarks of the first two generations,
a gluino octet and a massless neutralino, for squark or
gluino masses below 2 TeV, respectively. Squarks and gluinos
with equal masses below 1410 GeV are excluded. In minimal
supergravity/constrained minimal supersymmetric Standard
Model models with tanâ-¡β=10, A0=0 and μ>0, squarks and
gluinos of equal mass are excluded for masses below 1360
GeV. Constraints are also placed on the parameter space of
supersymmetric models with compressed spectra. These limits
considerably extend the region of supersymmetric parameter
space excluded by previous measurements with the ATLAS
detector.},
Doi = {10.1103/PhysRevD.87.012008},
Key = {fds307633}
}
@article{fds310367,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for squarks and gluinos with the ATLAS detector in
final states with jets and missing transverse momentum using
√s = 8 TeV proton-proton collision data},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {9},
Publisher = {Springer Nature},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2014)176},
Abstract = {A search for squarks and gluinos in final states containing
high-pTjets, missing transverse momentum and no electrons or
muons is presented. The data were recorded in 2012 by the
ATLAS experiment in √s = 8TeV proton-proton collisions at
the Large Hadron Collider, with a total integrated
luminosity of 20.3 fb−1. Results are interpreted in a
variety of simplified and specific supersymmetry-breaking
models assuming that R-parity is conserved and that the
lightest neutralino is the lightest supersymmetric particle.
An exclusion limit at the 95% confidence level on the mass
of the gluino is set at 1330GeV for a simplified model
incorporating only a gluino and the lightest neutralino. For
a simplified model involving the strong production of first-
and second-generation squarks, squark masses below 850GeV
(440GeV) are excluded for a massless lightest neutralino,
assuming mass degenerate (single light-flavour) squarks. In
mSUGRA/CMSSM models with tan β = 30, A0= −2m0and μ > 0,
squarks and gluinos of equal mass are excluded for masses
below 1700GeV. Additional limits are set for non-universal
Higgs mass models with gaugino mediation and for simplified
models involving the pair production of gluinos, each
decaying to a top squark and a top quark, with the top
squark decaying to a charm quark and a neutralino. These
limits extend the region of supersymmetric parameter space
excluded by previous searches with the ATLAS
detector.},
Doi = {10.1007/JHEP09(2014)176},
Key = {fds310367}
}
@article{fds313575,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
Title = {Search for standard model Higgs boson production in
association with a W boson at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {78},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2008},
Month = {August},
ISSN = {1550-7998},
url = {http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000258975300012&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=47d3190e77e5a3a53558812f597b0b92},
Abstract = {We present a search for standard model Higgs boson
production in association with a W boson in
proton-antiproton collisions (pp̄→ W±H→ νbb̄) at a
center of mass energy of 1.96 TeV. The search employs data
collected with the CDF II detector which correspond to an
integrated luminosity of approximately 1fb-1. We select
events consistent with a signature of a single lepton
(e±/μ±), missing transverse energy, and two jets. Jets
corresponding to bottom quarks are identified with a
secondary vertex tagging method and a neural network filter
technique. The observed number of events and the dijet mass
distributions are consistent with the standard model
background expectations, and we set 95% confidence level
upper limits on the production cross section times branching
ratio ranging from 3.9 to 1.3 pb for Higgs boson masses from
110 to 150GeV/c2, respectively. © 2008 The American
Physical Society.},
Doi = {10.1103/PhysRevD.78.032008},
Key = {fds313575}
}
@article{fds307808,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci,
MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
Title = {Search for standard model Higgs boson production in
association with a W boson using a matrix element technique
at CDF in pp̄ collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.85.072001},
Abstract = {This paper presents a search for standard model Higgs boson
production in association with a W boson using events
recorded by the CDF experiment in a data set corresponding
to an integrated luminosity of 5.6fb -1. The search is
performed using a matrix element technique in which the
signal and background hypotheses are used to create a
powerful discriminator. The discriminant output
distributions for signal and background are fit to the
observed events using a binned likelihood approach to search
for the Higgs boson signal. We find no evidence for a Higgs
boson, and 95% confidence level (C.L.) upper limits are set
on σ(pp̄→WH)×B(H→bb̄). The observed limits range
from 3.5 to 37.6 relative to the standard model expectation
for Higgs boson masses between m H=100GeV/c2 and m
H=150GeV/c2. The 95% C.L. expected limit is estimated from
the median of an ensemble of simulated experiments and
varies between 2.9 and 32.7 relative to the production rate
predicted by the standard model over the Higgs boson mass
range studied. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.85.072001},
Key = {fds307808}
}
@article{fds307997,
Author = {Aaltonen, T and others},
Title = {Search for standard model Higgs boson production in
association with a W boson using a neural network
discriminant at CDF},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {1},
Pages = {012002},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.012002},
Abstract = {We present a search for standard model Higgs boson
production in association with a W boson in
proton-antiproton collisions (pp̅ →W ±
H→ℓνbb̅ ) at a center of mass energy of 1.96 TeV. The
search employs data collected with the CDF II detector that
correspond to an integrated luminosity of approximately
1.9 fb-1. We select events consistent with a signature
of a single charged lepton (e ± /μ ± ),
missing transverse energy, and two jets. Jets corresponding
to bottom quarks are identified with a secondary vertex
tagging method, a jet probability tagging method, and a
neural network filter. We use kinematic information in an
artificial neural network to improve discrimination between
signal and background compared to previous analyses. The
observed number of events and the neural network output
distributions are consistent with the standard model
background expectations, and we set 95% confidence level
upper limits on the production cross section times branching
fraction ranging from 1.2 to 1.1 pb or 7.5 to 102 times the
standard model expectation for Higgs boson masses from 110
to 150 GeV/c2, respectively.},
Doi = {10.1103/PhysRevD.80.012002},
Key = {fds307997}
}
@article{fds356656,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede,
S},
Title = {Search for standard-model Z and Higgs bosons decaying into a
bottom-antibottom quark pair in proton-antiproton collisions
at 1.96 TeV SEARCH for STANDARD-MODEL Z and HIGGS ... T.
AALTONEN et al.},
Journal = {Physical Review D},
Volume = {98},
Number = {7},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.98.072002},
Abstract = {The Collider Detector at Fermilab collected a unique sample
of jets originating from bottom-quark fragmentation (b-jets)
by selecting online proton-antiproton (pp̄) collisions with
a vertex displaced from the pp̄ interaction point,
consistent with the decay of a bottom-quark hadron. This
data set, collected at a center-of-mass energy of 1.96 TeV,
and corresponding to an integrated luminosity of 5.4 fb-1,
is used to measure the Z-boson production cross section
times branching ratio into bb̄. The number of Z→bb̄
events is determined by fitting the dijet-mass distribution,
while constraining the dominant b-jet background,
originating from QCD multijet events, with data. The result,
σ(pp̄→Z)×B(Z→bb̄)=1.11±0.08(stat)±0.14(syst) nb,
is the most precise measurement of this process, and is
consistent with the standard-model prediction. The data set
is also used to search for Higgs-boson production. No
significant signal is expected in our data and the first
upper limit on the cross section for the inclusive
pp̄→H→bb̄ process at s=1.96 TeV is set, corresponding
to 33 times the expected standard-model cross section, or
σ=40.6 pb, at the 95% confidence level.},
Doi = {10.1103/PhysRevD.98.072002},
Key = {fds356656}
}
@article{fds356777,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M},
Title = {Search for strong gravity in multijet final states produced
in pp collisions at √s = 13 TeV using the ATLAS detector
at the LHC},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {3},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2016)026},
Abstract = {Abstract: A search is conducted for new physics in multijet
final states using 3.6 inverse femtobarns of data from
proton-proton collisions at (Formula presented.) TeV taken
at the CERN Large Hadron Collider with the ATLAS detector.
Events are selected containing at least three jets with
scalar sum of jet transverse momenta (HT) greater than 1
TeV. No excess is seen at large HTand limits are presented
on new physics: models which produce final states containing
at least three jets and having cross sections larger than
1.6 fb with HT> 5.8 TeV are excluded. Limits are also given
in terms of new physics models of strong gravity that
hypothesize additional space-time dimensions.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP03(2016)026},
Key = {fds356777}
}
@article{fds307767,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik,
E and Arik, M and Armbruster, AJ and Arnaez, O and Artamonov, A and Artoni,
G and Arutinov, D},
Title = {Search for strong gravity signatures in same-sign dimuon
final states using the ATLAS detector at the
LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {709},
Number = {4-5},
Pages = {322-340},
Publisher = {Elsevier BV},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2012.02.049},
Abstract = {A search for microscopic black holes has been performed in a
same-sign dimuon final state using 1.3 fb -1 of
proton-proton collision data collected with the ATLAS
detector at a centre of mass energy of 7 TeV at the CERN
Large Hadron Collider. The data are found to be consistent
with the expectation from the Standard Model and the results
are used to derive exclusion contours in the context of a
low scale gravity model. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.02.049},
Key = {fds307767}
}
@article{fds313589,
Author = {The, ATLASC and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek,
S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J},
Title = {Search for strong production of supersymmetric particles in
final states with missing transverse momentum and at least
three b-jets at (formula presented) TeV proton-proton
collisions with the ATLAS detector},
Journal = {Critical Ultrasound Journal},
Volume = {2014},
Number = {10},
Year = {2014},
Month = {January},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP10(2014)024},
Abstract = {© 2014, The Author(s). Abstract: This paper reports the
results of a search for strong production of supersymmetric
particles in 20.1 fb−1 of proton-proton collisions at a
centre-of-mass energy of 8 TeV using the ATLAS detector at
the LHC. The search is performed separately in events with
either zero or at least one high-pT lepton (electron or
muon), large missing transverse momentum, high jet
multiplicity and at least three jets identified as
originated from the fragmentation of a b-quark. No excess is
observed with respect to the Standard Model predictions. The
results are interpreted in the context of several
supersymmetric models involving gluinos and scalar top and
bottom quarks, as well as a mSUGRA/CMSSM model. Gluino
masses up to 1340 GeV are excluded, depending on the model,
significantly extending the previous ATLAS
limits.},
Doi = {10.1007/JHEP10(2014)024},
Key = {fds313589}
}
@article{fds315921,
Author = {Atlas Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman,
B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz,
K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio
Sola, JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet,
TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli,
M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerda Alberich and L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan,
SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal,
M},
Title = {Search for supersymmetry at [Formula: see text] TeV in
final states with jets and two same-sign leptons or three
leptons with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {5},
Pages = {259},
Year = {2016},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4095-8},
Abstract = {A search for strongly produced supersymmetric particles is
conducted using signatures involving multiple energetic jets
and either two isolated leptons (<i>e</i> or [Formula: see
text]) with the same electric charge or at least three
isolated leptons. The search also utilises <i>b</i>-tagged
jets, missing transverse momentum and other observables to
extend its sensitivity. The analysis uses a data sample of
proton-proton collisions at [Formula: see text] TeV
recorded with the ATLAS detector at the Large Hadron
Collider in 2015 corresponding to a total integrated
luminosity of 3.2 fb[Formula: see text]. No significant
excess over the Standard Model expectation is observed. The
results are interpreted in several simplified supersymmetric
models and extend the exclusion limits from previous
searches. In the context of exclusive production and
simplified decay modes, gluino masses are excluded at
[Formula: see text] confidence level up to 1.1-1.3 TeV for
light neutralinos (depending on the decay channel), and
bottom squark masses are also excluded up to 540 GeV. In the
former scenarios, neutralino masses are also excluded up to
550-850 GeV for gluino masses around 1 TeV.},
Doi = {10.1140/epjc/s10052-016-4095-8},
Key = {fds315921}
}
@article{fds310378,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Coutinho, YA and Amelung,
C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for supersymmetry at √s= 8 TeV in final states with
jets and two same-sign leptons or three leptons with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {6},
Publisher = {Springer Nature},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2014)035},
Abstract = {A search for strongly produced supersymmetric particles is
conducted using signatures involving multiple energetic jets
and either two isolated leptons (e or μ) with the same
electric charge, or at least three isolated leptons. The
search also utilises jets originating from b-quarks, missing
transverse momentum and other observables to extend its
sensitivity. The analysis uses a data sample corresponding
to a total integrated luminosity of 20.3 fb-1 of √s = 8
TeV proton-proton collisions recorded with the ATLAS
detector at the Large Hadron Collider in 2012. No deviation
from the Standard Model expectation is observed. New or
significantly improved exclusion limits are set on a wide
variety of supersymmetric models in which the lightest
squark can be of the first, second or third generations, and
in which R-parity can be conserved or violated. [Figure not
available: see fulltext.] © 2014 The Author(s).},
Doi = {10.1007/JHEP06(2014)035},
Key = {fds310378}
}
@article{fds321093,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali,
B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho,
YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso,
S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier,
S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper,
DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M},
Title = {Search for supersymmetry in a final state containing two
photons and missing transverse momentum in [Formula: see
text] = 13 TeV [Formula: see text] collisions at the LHC
using the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {9},
Pages = {517},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4344-x},
Abstract = {A search has been made for supersymmetry in a final state
containing two photons and missing transverse momentum using
the ATLAS detector at the Large Hadron Collider. The search
makes use of [Formula: see text] of proton-proton collision
data collected at a centre-of-mass energy of 13 TeV in
2015. Using a combination of data-driven and
Monte-Carlo-based approaches, the Standard Model background
is estimated to be [Formula: see text] events. No events are
observed in the signal region; considering the expected
background and its uncertainty, this observation implies a
model-independent 95 % CL upper limit of 0.93 fb (3.0
events) on the visible cross section due to physics beyond
the Standard Model. In the context of a generalized model of
gauge-mediated supersymmetry breaking with a bino-like
next-to-lightest supersymmetric particle, this leads to a
lower limit of 1650 GeV on the mass of a degenerate octet
of gluino states, independent of the mass of the lighter
bino-like neutralino.},
Doi = {10.1140/epjc/s10052-016-4344-x},
Key = {fds321093}
}
@article{fds313617,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
C},
Title = {Search for supersymmetry in events containing a same-flavour
opposite-sign dilepton pair, jets, and large missing
transverse momentum in [Formula: see text] TeV pp
collisions with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {318},
Year = {2015},
Month = {January},
ISSN = {1434-6044},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3518-2},
Abstract = {Two searches for supersymmetric particles in final states
containing a same-flavour opposite-sign lepton pair, jets
and large missing transverse momentum are presented. The
proton-proton collision data used in these searches were
collected at a centre-of-mass energy [Formula: see
text] TeV by the ATLAS detector at the Large Hadron
Collider and corresponds to an integrated luminosity of
20.3 fb[Formula: see text]. Two leptonic production
mechanisms are considered: decays of squarks and gluinos
with <i>Z</i> bosons in the final state, resulting in a peak
in the dilepton invariant mass distribution around the
<i>Z</i>-boson mass; and decays of neutralinos (e.g.
[Formula: see text]), resulting in a kinematic endpoint in
the dilepton invariant mass distribution. For the former, an
excess of events above the expected Standard Model
background is observed, with a significance of three
standard deviations. In the latter case, the data are
well-described by the expected Standard Model background.
The results from each channel are interpreted in the context
of several supersymmetric models involving the production of
squarks and gluinos.},
Doi = {10.1140/epjc/s10052-015-3518-2},
Key = {fds313617}
}
@article{fds356728,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for supersymmetry in events with b-tagged jets and
missing transverse momentum in pp collisions at √s=13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {11},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2017)195},
Abstract = {A search for the supersymmetric partners of the Standard
Model bottom and top quarks is presented. The search uses
36.1 fb−1 of pp collision data at s=13 TeV collected by
the ATLAS experiment at the Large Hadron Collider. Direct
production of pairs of bottom and top squarks (b¯ 1 and t¯
1) is searched for in final states with b-tagged jets and
missing transverse momentum. Distinctive selections are
defined with either no charged leptons (electrons or muons)
in the final state, or one charged lepton. The zero-lepton
selection targets models in which the b¯ 1 is the lightest
squark and decays via b¯1→bχ¯10, where χ¯10 is the
lightest neutralino. The one-lepton final state targets
models where bottom or top squarks are produced and can
decay into multiple channels, b¯1→bχ¯10 and b¯1→t or
t¯1→tχ¯10 and t¯1→b where χ¯1± is the lightest
chargino and the mass difference mχ¯1±−mχ¯10 is set
to 1 GeV. No excess above the expected Standard Model
background is observed. Exclusion limits at 95% confidence
level on the mass of third-generation squarks are derived in
various supersymmetry-inspired simplified
models.},
Doi = {10.1007/JHEP11(2017)195},
Key = {fds356728}
}
@article{fds366277,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal,
N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti,
C},
Title = {Search for supersymmetry in events with four or more charged
leptons in 139 fb −1 of √s = 13 TeV pp
collisions with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2021},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2021)167},
Abstract = {A search for supersymmetry in events with four or more
charged leptons (electrons, muons and τ-leptons) is
presented. The analysis uses a data sample corresponding to
139 fb−1 of proton-proton collisions delivered by the
Large Hadron Collider at s = 13 TeV and recorded by the
ATLAS detector. Four-lepton signal regions with up to two
hadronically decaying τ-leptons are designed to target
several supersymmetric models, while a general five-lepton
signal region targets any new physics phenomena leading to a
final state with five charged leptons. Data yields are
consistent with Standard Model expectations and results are
used to set upper limits on contributions from processes
beyond the Standard Model. Exclusion limits are set at the
95% confidence level in simplified models of general
gauge-mediated supersymmetry, excluding higgsino masses up
to 540 GeV. In R-parity-violating simplified models with
decays of the lightest supersymmetric particle to charged
leptons, lower limits of 1.6 TeV, 1.2 TeV, and 2.5 TeV are
placed on wino, slepton and gluino masses, respectively.
[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP07(2021)167},
Key = {fds366277}
}
@article{fds356670,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez,
O},
Title = {Search for supersymmetry in events with four or more leptons
in √s =13 TeV pp collisions with ATLAS},
Journal = {Physical Review D},
Volume = {98},
Number = {3},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.98.032009},
Abstract = {Results from a search for supersymmetry in events with four
or more charged leptons (electrons, muons and taus) are
presented. The analysis uses a data sample corresponding to
36.1 fb-1 of proton-proton collisions delivered by the Large
Hadron Collider at s=13 TeV and recorded by the ATLAS
detector. Four-lepton signal regions with up to two
hadronically decaying taus are designed to target a range of
supersymmetric scenarios that can be either enriched in or
depleted of events involving the production and decay of a Z
boson. Data yields are consistent with Standard Model
expectations and results are used to set upper limits on the
event yields from processes beyond the Standard Model.
Exclusion limits are set at the 95% confidence level in
simplified models of general gauge mediated supersymmetry,
where Higgsino masses are excluded up to 295 GeV. In
R-parity-violating simplified models with decays of the
lightest supersymmetric particle to charged leptons, lower
limits of 1.46, 1.06, and 2.25 TeV are placed on wino,
slepton and gluino masses, respectively.},
Doi = {10.1103/PhysRevD.98.032009},
Key = {fds356670}
}
@article{fds310361,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for supersymmetry in events with four or more leptons
in √s =8 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.90.052001},
Abstract = {Results from a search for supersymmetry in events with four
or more leptons including electrons, muons and taus are
presented. The analysis uses a data sample corresponding to
20.3 fb-1 of proton-proton collisions delivered by the Large
Hadron Collider at s=8 TeV and recorded by the ATLAS
detector. Signal regions are designed to target
supersymmetric scenarios that can be either enriched in or
depleted of events involving the production of a Z boson. No
significant deviations are observed in data from standard
model predictions and results are used to set upper limits
on the event yields from processes beyond the standard
model. Exclusion limits at the 95% confidence level on the
masses of relevant supersymmetric particles are obtained. In
R-parity-violating simplified models with decays of the
lightest supersymmetric particle to electrons and muons,
limits of 1350 and 750 GeV are placed on gluino and chargino
masses, respectively. In R-parity-conserving simplified
models with heavy neutralinos decaying to a massless
lightest supersymmetric particle, heavy neutralino masses up
to 620 GeV are excluded. Limits are also placed on other
supersymmetric scenarios.},
Doi = {10.1103/PhysRevD.90.052001},
Key = {fds310361}
}
@article{fds344667,
Author = {The ATLAS collaboration and A and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia, O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for supersymmetry in events with large missing
transverse momentum, jets, and at least one tau lepton in 20
fb−1 of √s= 8 TeV proton-proton collision data with the
ATLAS detector},
Journal = {Social Psychiatry and Psychiatric Epidemiology},
Volume = {2014},
Number = {9},
Publisher = {Dr. Dietrich Steinkopff Verlag GmbH and Co.
KG},
Year = {2014},
url = {http://dx.doi.org/10.1007/JHEP09(2014)103},
Abstract = {A search for supersymmetry (SUSY) in events with large
missing transverse momentum, jets, at least one hadronically
decaying tau lepton and zero or one additional light leptons
(electron/muon), has been performed using 20.3fb−1of
proton-proton collision data at √ s= 8 TeV recorded with
the ATLAS detector at the Large Hadron Collider. No excess
above the Standard Model background expectation is observed
in the various signal regions and 95% confidence level upper
limits on the visible cross section for new phenomena are
set. The results of the analysis are interpreted in several
SUSY scenarios, significantly extending previous limits
obtained in the same final states. In the framework of
minimal gauge-mediated SUSY breaking models, values of the
SUSY breaking scale Λ below 63 TeV are excluded,
independently of tan β. Exclusion limits are also derived
for an mSUGRA/CMSSM model, in both the R-parity-conserving
and R-parity-violating case. A further interpretation is
presented in a framework of natural gauge mediation, in
which the gluino is assumed to be the only light coloured
sparticle and gluino masses below 1090 GeV are
excluded.},
Doi = {10.1007/JHEP09(2014)103},
Key = {fds344667}
}
@article{fds307675,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Saavedra, JAA and Agustoni, M and Aharrouche,
M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Spiers, SEA and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
VV and Dos Santos and SPA and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik,
E},
Title = {Search for supersymmetry in events with large missing
transverse momentum, jets, and at least one tau lepton in 7
TeV proton-proton collision data with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {11},
Publisher = {Springer Nature},
Year = {2012},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2215-7},
Abstract = {A search for supersymmetry (SUSY) in events with large
missing transverse momentum, jets, and at least one
hadronically decaying τ lepton, with zero or one additional
light lepton (e/μ), has been performed using 4.7 fb−1of
proton-proton collision data at √s = 7 TeV recorded with
the ATLAS detector at the Large Hadron Collider. No excess
above the Standard Model background expectation is observed
and a 95 % confidence level visible cross-section upper
limit for new phenomena is set. In the framework of
gauge-mediated SUSY-breaking models, lower limits on the
mass scale Λ are set at 54 TeV in the regions where the
τ1is the next-to-lightest SUSY particle (tanβ > 20). These
limits provide the most stringent tests to date of GMSB
models in a large part of the parameter space
considered.},
Doi = {10.1140/epjc/s10052-012-2215-7},
Key = {fds307675}
}
@article{fds307623,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, L and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos,
S and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Mayes, JJB and Badescu, E and Bagnaia, P and Bahinipati,
S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio,
EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da
Costa, JBG and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Beemster, LJ and Begel, M and Harpaz,
SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni,
A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco,
M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blocki, J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boek, TT and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks,
WK and Brown, G and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez,
AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi,
G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Charlton, DG and Chavda,
V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B},
Title = {Search for supersymmetry in events with photons, bottom
quarks, and missing transverse momentum in proton-proton
collisions at a centre-of-mass energy of 7 TeV with the
ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {719},
Number = {4-5},
Pages = {261-279},
Publisher = {Elsevier BV},
Year = {2013},
url = {http://dx.doi.org/10.1016/j.physletb.2013.01.041},
Abstract = {© 2013 CERN A search has been performed for the
experimental signature of an isolated photon with high
transverse momentum, at least one jet identified as
originating from a bottom quark, and high missing transverse
momentum. Such a final state may originate from
supersymmetric models with gauge-mediated supersymmetry
breaking in events in which one of a pair of higgsino-like
neutralinos decays into a photon and a gravitino while the
other decays into a Higgs boson and a gravitino. The search
is performed using the full dataset of 7 TeV proton–proton
collisions recorded with the ATLAS detector at the LHC in
2011, corresponding to an integrated luminosity of 4.7
fb−1. A total of 7 candidate events are observed while
7.5±2.2 events are expected from the Standard Model
background. The results of the search are interpreted in the
context of general gauge mediation to exclude certain
regions of a benchmark plane for higgsino-like neutralino
production.},
Doi = {10.1016/j.physletb.2013.01.041},
Key = {fds307623}
}
@article{fds307696,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin,
DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone, G and Barr,
AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon,
P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova,
L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa,
HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard,
J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth,
CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini,
P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov,
O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Cherkaoui
El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot, J and Colon,
G and Conde Muiño and P and Coniavitis, E and Conidi,
MC},
Title = {Search for supersymmetry in events with three leptons and
missing transverse momentum in √[s]=7 TeV pp collisions
with the ATLAS detector.},
Journal = {Physical review letters},
Volume = {108},
Number = {26},
Pages = {261804},
Year = {2012},
Month = {June},
url = {http://dx.doi.org/10.1103/physrevlett.108.261804},
Abstract = {A search for the weak production of charginos and
neutralinos decaying to a final state with three leptons
(electrons or muons) and missing transverse momentum is
presented. The analysis uses 2.06 fb(-1) of √[s]=7 TeV
proton-proton collision data delivered by the Large Hadron
Collider and recorded with the ATLAS detector. Observations
are consistent with standard model expectations in two
signal regions that are either depleted or enriched in
Z-boson decays. Upper limits at 95% confidence level are set
in R-parity conserving phenomenological minimal
supersymmetric and simplified models. For the simplified
models, degenerate lightest chargino and next-to-lightest
neutralino masses up to 300 GeV are excluded for mass
differences from the lightest neutralino up to 300
GeV.},
Doi = {10.1103/physrevlett.108.261804},
Key = {fds307696}
}
@article{fds356664,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan,
O},
Title = {Search for supersymmetry in final states with charm jets and
missing transverse momentum in 13 TeV pp collisions with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {9},
Year = {2018},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2018)050},
Abstract = {A search for supersymmetric partners of top quarks decaying
as t˜1→cχ˜10 and supersymmetric partners of charm
quarks decaying as c˜1→cχ˜10, where χ˜10 is the
lightest neutralino, is presented. The search uses 36.1
fb−1pp collision data at a centre-of-mass energy of 13 TeV
collected by the ATLAS experiment at the Large Hadron
Collider and is performed in final states with jets
identified as containing charm hadrons. Assuming a 100%
branching ratio to cχ˜10, top and charm squarks with
masses up to 850 GeV are excluded at 95% confidence level
for a massless lightest neutralino. For mt˜1,c˜1−mχ˜10
< 100 GeV, top and charm squark masses up to 500 GeV are
excluded.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP09(2018)050},
Key = {fds356664}
}
@article{fds307743,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Search for supersymmetry in final states with jets, missing
transverse momentum and one isolated lepton in √s=7TeV pp
collisions using 1fb -1 of ATLAS
data},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012006},
Abstract = {We present an update of a search for supersymmetry in final
states containing jets, missing transverse momentum, and one
isolated electron or muon, using 1.04fb -1 of proton-proton
collision data at √s=7TeV recorded by the ATLAS experiment
at the LHC in the first half of 2011. The analysis is
carried out in four distinct signal regions with either
three or four jets and variations on the (missing)
transverse momentum cuts, resulting in optimized limits for
various supersymmetry models. No excess above the standard
model background expectation is observed. Limits are set on
the visible cross section of new physics within the
kinematic requirements of the search. The results are
interpreted as limits on the parameters of the minimal
supergravity framework, limits on cross sections of
simplified models with specific squark and gluino decay
modes, and limits on parameters of a model with bilinear
R-parity violation. © 2012 CERN.},
Doi = {10.1103/PhysRevD.85.012006},
Key = {fds307743}
}
@article{fds356682,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage,
LJ},
Title = {Search for supersymmetry in final states with missing
transverse momentum and multiple b-jets in proton-proton
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {6},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2018)107},
Abstract = {A search for supersymmetry involving the pair production of
gluinos decaying via third-generation squarks into the
lightest neutralino (χ˜10) is reported. It uses LHC
proton-proton collision data at a centre-of-mass energy s=13
TeV with an integrated luminosity of 36.1 fb−1 collected
with the ATLAS detector in 2015 and 2016. The search is
performed in events containing large missing transverse
momentum and several energetic jets, at least three of which
must be identified as originating from b-quarks. To increase
the sensitivity, the sample is divided into subsamples based
on the presence or absence of electrons or muons. No excess
is found above the predicted background. For χ˜10 masses
below approximately 300 GeV, gluino masses of less than 1.97
(1.92) TeV are excluded at 95% confidence level in
simplified models involving the pair production of gluinos
that decay via top (bottom) squarks. An interpretation of
the limits in terms of the branching ratios of the gluinos
into third-generation squarks is also provided. These
results improve upon the exclusion limits obtained with the
3.2 fb−1 of data collected in 2015.[Figure not available:
see fulltext.].},
Doi = {10.1007/JHEP06(2018)107},
Key = {fds356682}
}
@article{fds374215,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo
Ferraz, V and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Search for supersymmetry in final states with missing
transverse momentum and three or more b-jets in 139
fb-1 of proton–proton collisions at √s=13 TeV
with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {7},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11543-6},
Abstract = {A search for supersymmetry involving the pair production of
gluinos decaying via off-shell third-generation squarks into
the lightest neutralino (χ~10) is reported. It exploits LHC
proton–proton collision data at a centre-of-mass energy
s=13 TeV with an integrated luminosity of 139 fb - 1
collected with the ATLAS detector from 2015 to 2018. The
search uses events containing large missing transverse
momentum, up to one electron or muon, and several energetic
jets, at least three of which must be identified as
containing b-hadrons. Both a simple kinematic event
selection and an event selection based upon a deep
neural-network are used. No significant excess above the
predicted background is found. In simplified models
involving the pair production of gluinos that decay via
off-shell top (bottom) squarks, gluino masses less than
2.44 TeV (2.35 TeV) are excluded at 95% CL for a massless
χ~10. Limits are also set on the gluino mass in models with
variable branching ratios for gluino decays to
bb¯χ~10,tt¯χ~10 and tb¯χ~1-/t¯bχ~1+.},
Doi = {10.1140/epjc/s10052-023-11543-6},
Key = {fds374215}
}
@article{fds356738,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid, OS and Abraham,
NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya,
BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco,
P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for supersymmetry in final states with two same-sign
or three leptons and jets using 36 fb−1 of
√s=13 TeV pp collision data with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {9},
Year = {2017},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2017)084},
Abstract = {A search for strongly produced supersymmetric particles
using signatures involving multiple energetic jets and
either two isolated same-sign leptons (e or μ), or at least
three isolated leptons, is presented. The analysis relies on
the identification of b-jets and high missing transverse
momentum to achieve good sensitivity. A data sample of
proton-proton collisions at s=13 TeV recorded with the ATLAS
detector at the Large Hadron Collider in 2015 and 2016,
corresponding to a total integrated luminosity of 36.1
fb−1, is used for the search. No significant excess over
the Standard Model prediction is observed. The results are
interpreted in several simplified supersymmetric models
featuring R-parity conservation or R-parity violation,
extending the exclusion limits from previous searches. In
models considering gluino pair production, gluino masses are
excluded up to 1.87 TeV at 95% confidence level. When bottom
squarks are pair-produced and decay to a chargino and a top
quark, models with bottom squark masses below 700 GeV and
light neutralinos are excluded at 95% confidence level. In
addition, model-independent limits are set on a possible
contribution of new phenomena to the signal region
yields.[Figure not available: see fulltext.].},
Doi = {10.1007/JHEP09(2017)084},
Key = {fds356738}
}
@article{fds307782,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Search for supersymmetry in pp collisions at √s=7TeV in
final states with missing transverse momentum and b-jets
with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.85.112006},
Abstract = {The results of a search for supersymmetry in events with
large missing transverse momentum and heavy-flavor jets
using an integrated luminosity corresponding to 2.05fb-1 of
pp collisions at √s=7TeV recorded with the ATLAS detector
at the Large Hadron Collider are reported. No significant
excess is observed with respect to the prediction for
standard model processes. Results are interpreted in a
variety of R-parity conserving models in which scalar
bottoms and tops are the only scalar quarks to appear in the
gluino decay cascade, and in an SO(10) model framework.
Gluino masses up to 600-900GeV are excluded, depending on
the model considered. © 2012 CERN. Published by the
American Physical Society.},
Doi = {10.1103/PhysRevD.85.112006},
Key = {fds307782}
}
@article{fds308002,
Author = {Aaltonen, T and others},
Title = {Search for Supersymmetry in pp̅ Collisions at √ s
=1.96 TeV Using the Trilepton Signature for
Chargino-Neutralino Production},
Journal = {Physical Review Letters},
Volume = {101},
Number = {25},
Pages = {251801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.251801},
Abstract = {We use the three lepton and missing energy trilepton
signature to search for chargino-neutralino production with
2.0 fb-1 of integrated luminosity collected by the CDF
II experiment at the Tevatron pp̅ collider. We expect an
excess of approximately 11 supersymmetric events for a
choice of parameters of the mSUGRA model, but our
observation of 7 events is consistent with the standard
model expectation of 6.4 events. We constrain the mSUGRA
model of supersymmetry and rule out chargino masses up to
145 GeV/c2 for a specific choice of
parameters.},
Doi = {10.1103/physrevlett.101.251801},
Key = {fds308002}
}
@article{fds308137,
Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, J-L and Ahmed, SN and Ahn,
SH and Alexeev, GD and Alkhazov, G and Alton, A and Alverson, G and Alves,
GA and Anderson, S and Andrieu, B and Arnoud, Y and Askew, A and Asman, B and Atramentov, O and Autermann, C and Avila, C and Babukhadia, L and Bacon,
TC and Baden, A and Baffioni, S and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Bargassa, P and Baringer, P and Barnes, C and Barreto,
J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beauceron,
S and Beaudette, F and Begel, M and Bellavance, A and Beri, SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Besson,
A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Binder, M and Bischoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Bloch, D and Blumenschein,
U and Boehnlein, A and Boeriu, O and Bolton, TA and Bonamy, P and Borcherding, F and Borissov, G and Bos, K and Bose, T and Boswell, C and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchanan, NJ and Buchholz, D and Buehler, M and Buescher, V and Burdin,
S and Burnett, TH and Busato, E and Butler, JM and Bystricky, J and Canelli, F and Carvalho, W and Casey, BCK and Casey, D and Cason, NM and Castilla-Valdez, H and Chakrabarti, S and Chakraborty, D and Chan,
KM and Chandra, A and Chapin, D and Charles, F and Cheu, E and Chevalier,
L and Cho, DK and Choi, S and Chopra, S and Christiansen, T and Christofek,
L and Claes, D and Clark, AR and Clément, B and Clément, C and Coadou, Y and Colling, DJ and Coney, L and Connolly, B and Cooke, M and Cooper, WE and Coppage, D and Corcoran, M and Coss, J and Cothenet, A and Cousinou,
M-C and Crépé-Renaudin, S and Cristetiu, M and Cummings, MAC and Cutts, D and da Motta, H and Davies, B and Davies, G and Davis, GA and De,
K and de Jong, P and de Jong, SJ and De La Cruz-Burelo and E and De
Oliveira Martins and C and Dean, S and Del Signore and K and Déliot, F and Delsart, PA and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doidge, M and Dong, H and Doulas, S and Duflot, L and Dugad, SR and Duperrin, A and Dyer,
J and Dyshkant, A and Eads, M and Edmunds, D and Edwards, T and Ellison, J and Elmsheuser, J and Eltzroth, JT and Elvira, VD and Eno, S and Ermolov, P and Eroshin, OV and Estrada, J and Evans, D and Evans, H and Evdokimov, A and Evdokimov, VN and Fast, J and Fatakia, SN and Fein, D and Feligioni, L and Ferbel, T and Fiedler, F and Filthaut, F and Fisher, W and Fisk, HE and Fleuret, F and Fortner, M and Fox, H and Freeman, W and Fu, S and Fuess, S and Galea, CF and Gallas, E and Galyaev, E and Gao, M and Garcia, C and Garcia-Bellido, A and Gardner, J and Gavrilov, V and Gelé, D and Gelhaus, R and Genser, K and Gerber, CE and Gershtein, Y and Geurkov, G and Ginther, G and Goldmann, K and Golling, T and Gómez, B and Gounder, K and Goussiou, A and Graham, G and Grannis, PD and Greder, S and Green, JA and Greenlee, H and Greenwood, ZD and Gregores, EM and Grinstein, S and Grivaz, J-F and Groer, L and Grünendahl, S and Grünewald, MW and Gu,
W and Gurzhiev, SN and Gutierrez, G and Gutierrez, P and Haas, A and Hadley, NJ and Haggerty, H and Hagopian, S and Hall, I and Hall, RE and Han, C and Han, L and Hanagaki, K and Hanlet, P and Harder, K and Harrington, R and Hauptman, JM and Hauser, R and Hays, C and Hays, J and Hebbeker, T and Hebert, C and Hedin, D and Heinmiller, JM and Heinson,
AP and Heintz, U and Hensel, C and Hesketh, G and Hildreth, MD and Hirosky,
R and Hobbs, JD and Hoeneisen, B and Hohlfeld, M and Hong, SJ and Hooper,
R and Hou, S and Hu, Y and Huang, J and Huang, Y and Iashvili, I and Illingworth, R and Ito, AS and Jabeen, S and Jaffré, M and Jain, S and Jain, V and Jakobs, K and Jenkins, A and Jesik, R and Jiang, Y and Johns,
K and Johnson, M and Johnson, P and Jonckheere, A and Jonsson, P and Jöstlein, H and Juste, A and Kado, MM and Käfer, D and Kahl, W and Kahn,
S and Kajfasz, E and Kalinin, AM and Kalk, J and Karmanov, D and Kasper, J and Kau, D and Ke, Z and Kehoe, R and Kermiche, S and Kesisoglou, S and Khanov,
A and Kharchilava, A and Kharzheev, YM and Kim, KH and Klima, B and Klute,
M and Kohli, JM and Kopal, M and Korablev, VM and Kotcher, J and Kothari,
B and Kotwal, AV and Koubarovsky, A and Kouchner, A and Kouznetsov, O and Kozelov, AV and Kozminski, J and Krane, J and Krishnaswamy, MR and Krzywdzinski, S and Kubantsev, M and Kuleshov, S and Kulik, Y and Kunori, S and Kupco, A and Kurca, T and Kuznetsov, VE and Lager, S and Lahrichi, N and Landsberg, G and Lazoflores, J and Le Bihan and A-C and Lebrun, P and Lee, SW and Lee, WM and Leflat, A and Leggett, C and Lehner,
F and Leonidopoulos, C and Lewis, P and Li, J and Li, QZ and Li, X and Lima,
JGR and Lincoln, D and Linn, SL and Linnemann, J and Lipaev, VV and Lipton,
R and Lobo, L and Lobodenko, A and Lokajicek, M and Lounis, A and Lu, J and Lubatti, HJ and Lucotte, A and Lueking, L and Luo, C and Lynker, M and Lyon, AL and Maciel, AKA and Madaras, RJ and Mättig, P and Magerkurth,
A and Magnan, A-M and Maity, M and Mal, PK and Malik, S and Malyshev, VL and Manankov, V and Mao, HS and Maravin, Y and Marshall, T and Martens, M and Martin, MI and Mattingly, SEK and Mayorov, AA and McCarthy, R and McCroskey, R and McMahon, T and Meder, D and Melanson, HL and Melnitchouk, A and Meng, X and Merkin, M and Merritt, KW and Meyer, A and Miao, C and Miettinen, H and Mihalcea, D and Mishra, CS and Mitrevski,
J and Mokhov, N and Molina, J and Mondal, NK and Montgomery, HE and Moore,
RW and Mostafa, M and Muanza, GS and Mulders, M and Mutaf, YD and Nagy, E and Nang, F and Narain, M and Narasimham, VS and Naumann, NA and Neal, HA and Negret, JP and Nelson, S and Neustroev, P and Noeding, C and Nomerotski,
A and Novaes, SF and Nunnemann, T and Nurse, E and O'Dell, V and O'Neil,
DC and Oguri, V and Oliveira, N and Olivier, B and Oshima, N and Otero y
Garzón, GJ and Padley, P and Papageorgiou, K and Parashar, N and Park,
J and Park, SK and Parsons, J and Partridge, R and Parua, N and Patwa, A and Perea, PM and Perez, E and Peters, O and Pétroff, P and Petteni, M and Phaf, L and Piegaia, R and Podesta-Lerma, PLM and Podstavkov, VM and Pope, BG and Popkov, E and Prado da Silva and WL and Prosper, HB and Protopopescu, S and Przybycien, MB and Qian, J and Quadt, A and Quinn,
B and Rani, KJ and Rapidis, PA and Ratoff, PN and Reay, NW and Renardy,
J-F and Reucroft, S and Rha, J and Ridel, M and Rijssenbeek, M and Ripp-Baudot, I and Rizatdinova, F and Royon, C and Rubinov, P and Ruchti, R and Sabirov, BM and Sajot, G and Sánchez-Hernández, A and Sanders, MP and Santoro, A and Savage, G and Sawyer, L and Scanlon, T and Schamberger, RD and Schellman, H and Schieferdecker, P and Schmitt,
C and Schukin, AA and Schwartzman, A and Schwienhorst, R and Sengupta,
S and Severini, H and Shabalina, E and Shary, V and Shephard, WD and Shpakov, D and Sidwell, RA and Simak, V and Sirotenko, V and Skow, D and Skubic, P and Slattery, P and Smith, RP and Smolek, K and Snow, GR and Snow, J and Snyder, S and Söldner-Rembold, S and Song, X and Song, Y and Sonnenschein, L and Sopczak, A and Sorín, V and Sosebee, M and Soustruznik, K and Souza, M and Spurlock, B and Stanton, NR and Stark,
J and Steele, J and Steinbrück, G and Stevenson, K and Stolin, V and Stone, A and Stoyanova, DA and Strandberg, J},
Title = {Search for supersymmetry with gauge-mediated breaking in
diphoton events at D0.},
Journal = {Physical review letters},
Volume = {94},
Number = {4},
Pages = {041801},
Year = {2005},
Month = {February},
url = {http://dx.doi.org/10.1103/physrevlett.94.041801},
Abstract = {We report the results of a search for supersymmetry (SUSY)
with gauge-mediated breaking in the missing transverse
energy distribution of inclusive diphoton events using 263
pb(-1) of data collected by the D0 experiment at the
Fermilab Tevatron Collider in 2002-2004. No excess is
observed above the background expected from standard model
processes, and lower limits on the masses of the lightest
neutralino and chargino of about 108 and 195 GeV,
respectively, are set at the 95% confidence level. These are
the most stringent limits to date for models with
gauge-mediated SUSY breaking with a short-lived neutralino
as the next-to-lightest SUSY particle.},
Doi = {10.1103/physrevlett.94.041801},
Key = {fds308137}
}
@article{fds307913,
Author = {Aaltonen, and T, and others},
Title = {Search for Supersymmetry with Gauge-Mediated Breaking in
Diphoton Events with Missing Transverse Energy at CDF
II},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {1},
Pages = {011801},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.011801},
Abstract = {http://arxiv.org/abs/0910.3606},
Doi = {10.1103/PhysRevLett.104.011801},
Key = {fds307913}
}
@article{fds307779,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ},
Title = {Search for supersymmetry with jets, missing transverse
momentum and at least one hadronically decaying τ lepton in
proton-proton collisions at s=7TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {714},
Number = {2-5},
Pages = {197-214},
Publisher = {Elsevier BV},
Year = {2012},
Month = {August},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.06.061},
Abstract = {A search for production of supersymmetric particles in final
states containing jets, missing transverse momentum, and at
least one hadronically decaying τ lepton is presented. The
data were recorded by the ATLAS experiment in s=7TeV
proton-proton collisions at the Large Hadron Collider. No
excess above the Standard Model background expectation was
observed in 2.05fb-1 of data. The results are interpreted in
the context of gauge mediated supersymmetry breaking models
with Mmess=250TeV, N5=3, μ>0, and Cgrav=1. The production
of supersymmetric particles is excluded at 95% C.L. up to a
supersymmetry breaking scale Λ=30TeV, independent of tanβ,
and up to Λ=43TeV for large tanβ. © 2012.},
Doi = {10.1016/j.physletb.2012.06.061},
Key = {fds307779}
}
@article{fds307653,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and d'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Eusebi, R and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da
Costa, J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker, A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim,
DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Knoepfel, K and Kondo, K and Kong,
DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucà, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, P and Martínez, M and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi,
N and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus, C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Ranjan, N and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and Stancari, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez, F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson,
P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF Collaboration},
Title = {Search for supersymmetry with like-sign lepton-tau events at
CDF.},
Journal = {Physical review letters},
Volume = {110},
Number = {20},
Pages = {201802},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.110.201802},
Abstract = {We present a search for chargino-neutralino associated
production using like electric charge dilepton events
collected by the CDF II detector at the Fermilab Tevatron in
proton-antiproton collisions at sqrt[s] = 1.96 TeV. One
lepton is identified as the hadronic decay of a tau lepton,
while the other is an electron or muon. In data
corresponding to 6.0 fb(-1) of integrated luminosity, we
obtain good agreement with standard model predictions and
set limits on the chargino-neutralino production cross
section for simplified gravity- and gauge-mediated models.
As an example, assuming that the chargino and neutralino
decays to taus dominate, in the simplified gauge-mediated
model we exclude cross sections greater than 300 fb at 95%
credibility level for chargino and neutralino masses of 225
GeV/c(2). This analysis is the first to extend the LHC
searches for electroweak supersymmetric production of
gauginos to high tanβ and slepton next-to-lightest
supersymmetric particle scenarios.},
Doi = {10.1103/physrevlett.110.201802},
Key = {fds307653}
}
@article{fds307689,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates,
RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera,
PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendel, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund,
E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry,
T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas,
CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen,
X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
Title = {Search for tb resonances in proton-proton collisions at
√s=7 TeV with the ATLAS detector.},
Journal = {Physical review letters},
Volume = {109},
Number = {8},
Pages = {081801},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.109.081801},
Abstract = {This Letter presents a search for tb resonances in 1.04
fb(-1) of LHC proton-proton collision data collected by the
ATLAS detector at a center-of-mass energy of 7 TeV. Events
with a lepton, missing transverse momentum, and two jets are
selected and the invariant mass of the corresponding final
state is reconstructed. The search exploits the shape of the
tb invariant mass distribution compared to the expected
standard model backgrounds. The model of a right-handed
W(R)' with standard model-like couplings is chosen as the
benchmark model for this search. No statistically
significant excess of events is observed in the data, and
upper limits on the cross section times the branching ratio
of W(R)' resonances at 95% C.L. lie in the range of 6.1-1.0
pb for W(R)' masses ranging from 0.5 to 2.0 TeV. These
limits are translated into a lower bound on the allowed
right-handed W(R)' mass, giving m(W(R)'))>1.13 TeV at 95%
C.L.},
Doi = {10.1103/physrevlett.109.081801},
Key = {fds307689}
}
@article{fds307907,
Author = {Aaltonen, and T, and others},
Title = {Search for Technicolor Particles Produced in Association
with a $W$ Boson at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {104},
Number = {11},
Pages = {111802},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.104.111802},
Abstract = {http://arxiv.org/abs/0912.2059},
Doi = {10.1103/PhysRevLett.104.111802},
Key = {fds307907}
}
@article{fds307724,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ami, SB and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli,
EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger,
N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani,
G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW},
Title = {Search for TeV-scale gravity signatures in final states with
leptons and jets with the ATLAS detector at √ s=7
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {716},
Number = {1},
Pages = {122-141},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.08.009},
Abstract = {The production of events with multiple high transverse
momentum particles including charged leptons and jets is
measured, using 1.04 fb-1 of proton-proton collision data
recorded by the ATLAS detector during the first half of 2011
at √s=7 TeV. No excess beyond Standard Model expectations
is observed, and upper limits on the fiducial cross sections
for non-Standard Model production of these final states are
set. Using models for string ball and black hole production
and decay, exclusion contours are determined as a function
of mass threshold and the fundamental gravity scale. © 2012
CERN.},
Doi = {10.1016/j.physletb.2012.08.009},
Key = {fds307724}
}
@article{fds321087,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for TeV-scale gravity signatures in high-mass final
states with leptons and jets with the ATLAS detector at
√s=13 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {760},
Pages = {520-537},
Publisher = {Elsevier BV},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1016/j.physletb.2016.07.030},
Abstract = {A search for physics beyond the Standard Model, in final
states with at least one high transverse momentum charged
lepton (electron or muon) and two additional high transverse
momentum leptons or jets, is performed using 3.2 fb−1 of
proton–proton collision data recorded by the ATLAS
detector at the Large Hadron Collider in 2015 at s=13 TeV.
The upper end of the distribution of the scalar sum of the
transverse momenta of leptons and jets is sensitive to the
production of high-mass objects. No excess of events beyond
Standard Model predictions is observed. Exclusion limits are
set for models of microscopic black holes with two to six
extra dimensions.},
Doi = {10.1016/j.physletb.2016.07.030},
Key = {fds321087}
}
@article{fds313599,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for the associated production of the Higgs boson with
a top quark pair in multilepton final states with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {749},
Pages = {519-541},
Publisher = {Elsevier BV},
Year = {2015},
Month = {October},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2015.07.079},
Abstract = {A search for the associated production of the Higgs boson
with a top quark pair is performed in multilepton final
states using 20.3 fb−1 of proton–proton collision data
recorded by the ATLAS experiment at s=8 TeV at the Large
Hadron Collider. Five final states, targeting the decays
H→WW⁎, ττ, and ZZ⁎, are examined for the presence of
the Standard Model (SM) Higgs boson: two same-charge light
leptons (e or μ) without a hadronically decaying τ lepton;
three light leptons; two same-charge light leptons with a
hadronically decaying τ lepton; four light leptons; and one
light lepton and two hadronically decaying τ leptons. No
significant excess of events is observed above the
background expectation. The best fit for the tt¯H
production cross section, assuming a Higgs boson mass of 125
GeV, is 2.1−1.2+1.4 times the SM expectation, and the
observed (expected) upper limit at the 95% confidence level
is 4.7 (2.4) times the SM rate. The p-value for
compatibility with the background-only hypothesis is 1.8σ;
the expectation in the presence of a Standard Model signal
is 0.9σ.},
Doi = {10.1016/j.physletb.2015.07.079},
Key = {fds313599}
}
@article{fds307936,
Author = {Aaltonen, T and others},
Title = {Search for the Associated Production of the Standard-Model
Higgs Boson in the All-Hadronic Channel},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {22},
Pages = {221801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.221801},
Abstract = {We report on a search for the standard-model Higgs boson in
pp̅ collisions at sqrt[s]=1.96 TeV using an integrated
luminosity of 2.0 fb-1. We look for production of the
Higgs boson decaying to a pair of bottom quarks in
association with a vector boson V (W or Z) decaying to
quarks, resulting in a four-jet final state. Two of the jets
are required to have secondary vertices consistent with
B-hadron decays. We set the first 95% confidence level upper
limit on the VH production cross section with V(→qq̅
/qq′)H(→bb̅ ) decay for Higgs boson masses of
100--150 GeV/c2 using data from run II at the Fermilab
Tevatron. For mH=120 GeV/c2, we exclude cross sections
larger than 38 times the standard-model prediction.},
Doi = {10.1103/physrevlett.103.221801},
Key = {fds307936}
}
@article{fds310325,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for the b¯b decay of the Standard Model Higgs boson
in associated (W/Z)H production with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {1},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2015)069},
Abstract = {Abstract: A search for the (Formula presented.) decay of the
Standard Model Higgs boson is performed with the ATLAS
experiment using the full dataset recorded at the LHC in Run
1. The integrated luminosities used are 4.7 and 20.3 fb−1
from pp collisions at (Formula presented.) and 8 TeV,
respectively. The processes considered are associated (W/Z)H
production, where W → eν/μν, Z → ee/μμ and Z →
νν. The observed (expected) deviation from the
background-only hypothesis corresponds to a significance of
1.4 (2.6) standard deviations and the ratio of the measured
signal yield to the Standard Model expectation is found to
be μ = 0.52 ± 0.32 (stat.) ± 0.24 (syst.) for a Higgs
boson mass of 125.36 GeV. The analysis procedure is
validated by a measurement of the yield of (W/Z)Z production
with (Formula presented.) in the same final states as for
the Higgs boson search, from which the ratio of the observed
signal yield to the Standard Model expectation is found to
be 0.74 ± 0.09 (stat.) ± 0.14 (syst.).[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP01(2015)069},
Key = {fds310325}
}
@article{fds373911,
Author = {Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Sharma, AS and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk Cakir and I and Sultansoy, S and Adam Bourdarios and C and Belfkir, M and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Franco, L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Lafaye, R and Levêque, J and Lorenzo Martinez and N and Portales, L and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Wingerter-Seez, I and Abulaiti, Y and Bhopatkar, VS and Chekanov, S and Darmora, S and Hopkins, WH and Kourlitis, E and LeCompte, T and Love, J and Metcalfe,
J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Zhang, J and Berlendis, S and Cheu, E and Delitzsch, CM and Johns, KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas,
JCJ and De, K and Eifert, T and Farbin, A and Hadavand, HK and Little, JD and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Gazis, EN and Gkountoumis, P and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Perini, L and Tzanis, P and Zacharis, G and Andeen, T and Burton, CD and Choi, K and Nikiforou, N and Onyisi, PUE and Panchal, DK and Roy, A and Unal, M and Webb, AF and Beddall, AJ and Celebi, E},
Title = {Search for the charged-lepton-flavor-violating decay Z →
eμ in pp collisions at √s = 13 TeV ATLAS
detector},
Journal = {Physical Review D},
Volume = {108},
Number = {3},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.108.032015},
Abstract = {A search for the charged-lepton-flavor-violating process
Formula Presented is presented, using Formula Presented of
Formula Presented Formula Presented collision data collected
by the ATLAS experiment at the LHC. An excess in the Formula
Presented invariant mass spectrum near the Formula Presented
boson mass would be a striking signature of new physics. No
excess is observed, and an upper limit Formula Presented is
placed on the branching fraction at 95% confidence level,
which is the most stringent limit to date.},
Doi = {10.1103/PhysRevD.108.032015},
Key = {fds373911}
}
@booklet{Abbott98i,
Author = {B. Abbott and M. Abolins and B. S. Acharya and I. Adam and D. L. Adams and M. Adams and S. Ahn and H. Aihara and G. A.
Alves and N. Amos and E. W. Anderson and R. Astur and M. M.
Baarmand and A. Baden and V. Balamurali and J. Balderston and B. Baldin and},
Title = {Search for the decay b -$>$ X-s mu(+)mu(-)},
Journal = {Physics Letters B},
Volume = {423},
Number = {3-4},
Pages = {419 -- 426},
Year = {1998},
Month = {March},
Key = {Abbott98i}
}
@article{fds313624,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan,
K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau,
M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio,
EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa,
JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin,
M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham,
M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz, SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek,
T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein,
U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni,
S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun,
HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans,
G and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins, NJ and Collins-Tooth, C and Collot,
J and Colon, G and Muiño, PC and Coniavitis, E and Conidi, MC and Consonni, SM and Consorti, V},
Title = {Search for the decay Bs0→μ+μ-
with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {713},
Number = {4-5},
Pages = {387-407},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.06.013},
Abstract = {A blind analysis searching for the decay Bs0→μ+μ- has
been performed using proton-proton collisions at a
centre-of-mass energy of 7 TeV recorded with the ATLAS
detector at the LHC. With an integrated luminosity of 2.4
fb-1 no excess of events over the background expectation is
found and an upper limit is set on the branching fraction
BR(Bs0→μ+μ-)<2.2(1.9)×10-8 at 95% (90%) confidence
level. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.06.013},
Key = {fds313624}
}
@article{fds376246,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Search for the decay of the Higgs boson to a Z boson and a
light pseudoscalar particle decaying to two
photons},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {850},
Year = {2024},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2024.138536},
Abstract = {A search for the decay of the Higgs boson to a Z boson and a
light, pseudoscalar particle, a, decaying respectively to
two leptons and to two photons is reported. The search uses
the full LHC Run 2 proton–proton collision data at s=13
TeV, corresponding to 139 fb−1 collected by the ATLAS
detector. This is one of the first searches for this
specific decay mode of the Higgs boson, and it probes
unexplored parameter space in models with axion-like
particles (ALPs) and extended scalar sectors. The mass of
the a particle is assumed to be in the range 0.1–33 GeV.
The data are analysed in two categories: a merged category
where the photons from the a decay are reconstructed in the
ATLAS calorimeter as a single cluster, and a resolved
category in which two separate photons are detected. The
main background processes are from Standard Model Z boson
production in association with photons or jets. The data are
in agreement with the background predictions, and upper
limits on the branching ratio of the Higgs boson decay to Za
times the branching ratio a→γγ are derived at the 95%
confidence level and they range from 0.08% to 2% depending
on the mass of the a particle. The results are also
interpreted in the context of ALP models.},
Doi = {10.1016/j.physletb.2024.138536},
Key = {fds376246}
}
@article{fds347461,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
J-F and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
JT and Bajic, M and Baker, OK and Bakker, PJ and Bakshi Gupta and D and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnea,
R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Belyaev, NL and Benary,
O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertram, IA and Bertsche, C and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini,
C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black,
JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, D and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boerner,
D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona,
M and Bonilla, JS and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow,
TM and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher,
D and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar,
CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano
Bret, M and Cantero, J and Cao, T and Cao, Y and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli,
R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin, E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casha, AF and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Cinca, D and Cindro, V and Cioară,
IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Clark,
A and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M},
Title = {Search for the Decay of the Higgs Boson to Charm Quarks with
the ATLAS Experiment.},
Journal = {Physical review letters},
Volume = {120},
Number = {21},
Pages = {211802},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.120.211802},
Abstract = {A direct search for the standard model Higgs boson decaying
to a pair of charm quarks is presented. Associated
production of the Higgs and Z bosons, in the decay mode
ZH→ℓ^{+}ℓ^{-}cc[over ¯] is studied. A data set with
an integrated luminosity of 36.1 fb^{-1} of pp
collisions at sqrt[s]=13TeV recorded by the ATLAS experiment
at the LHC is used. The H→cc[over ¯] signature is
identified using charm-tagging algorithms. The observed
(expected) upper limit on σ(pp→ZH)×B(H→cc[over ¯]) is
2.7 (3.9_{-1.1}^{+2.1}) pb at the 95% confidence level for
a Higgs boson mass of 125 GeV, while the standard model
value is 26 fb.},
Doi = {10.1103/physrevlett.120.211802},
Key = {fds347461}
}
@article{fds307952,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, P-H and Bedeschi, F and Beecher,
D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman, A and Brigliadori, L and Bromberg,
C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burke, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Chwalek, T and Ciobanu, CI and Ciocci, MA and Clark,
A and Clark, D and Compostella, G and Convery, ME and Conway, J and Cordelli, M and Cortiana, G and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R and Cully, JC and Dagenhart, D and Datta, M and Davies, T and de Barbaro, P and De Cecco,
S and Deisher, A and De Lorenzo and G and Dell'orso, M and Deluca, C and Demortier, L and Deng, J and Deninno, M and Derwent, PF and di Giovanni,
GP and Dionisi, C and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong, P and Donini, J and Dorigo, T and Dube, S and Efron, J and Elagin, A and Erbacher, R and Errede, D and Errede, S and Eusebi, R and Fang, HC and Farrington, S and Fedorko, WT and Feild, RG and Feindt, M and Fernandez, JP and Ferrazza, C and Field, R and Flanagan, G and Forrest,
R and Frank, MJ and Franklin, M and Freeman, JC and Furic, I and Gallinaro,
M and Galyardt, J and Garberson, F and Garcia, JE and Garfinkel, AF and Genser, K and Gerberich, H and Gerdes, D and Gessler, A and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Gimmell, JL and Ginsburg, CM and Giokaris, N and Giordani, M and Giromini, P and Giunta,
M and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold, M and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Gresele, A and Grinstein, S and Grosso-Pilcher, C and Grundler, U and Guimaraes da Costa and J and Gunay-Unalan, Z and Haber,
C and Hahn, K and Hahn, SR and Halkiadakis, E and Han, B-Y and Han, JY and Happacher, F and Hara, K and Hare, D and Hare, M and Harper, S and Harr,
RF and Harris, RM and Hartz, M and Hatakeyama, K and Hays, C and Heck, M and Heijboer, A and Heinrich, J and Henderson, C and Herndon, M and Heuser,
J and Hewamanage, S and Hidas, D and Hill, CS and Hirschbuehl, D and Hocker, A and Hou, S and Houlden, M and Hsu, S-C and Huffman, BT and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Incandela,
J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jha, MK and Jindariani, S and Johnson, W and Jones, M and Joo, KK and Jun, SY and Jung, JE and Junk, TR and Kamon, T and Kar, D and Karchin, PE and Kato, Y and Kephart, R and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, HW and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kimura, N and Kirsch, L and Klimenko, S and Knuteson, B and Ko, BR and Kondo, K and Kong,
DJ and Konigsberg, J and Korytov, A and Kotwal, AV and Kreps, M and Kroll,
J and Krop, D and Krumnack, N and Kruse, M and Krutelyov, V and Kubo, T and Kuhr, T and Kulkarni, NP and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and Lazzizzera, I and Lecompte, T and Lee, E and Lee,
HS and Lee, SW and Leone, S and Lewis, JD and Lin, C-S and Linacre, J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, T and Lockyer, NS and Loginov, A and Loreti, M and Lovas, L and Lucchesi, D and Luci, C and Lueck, J and Lujan, P and Lukens, P and Lungu,
G and Lyons, L and Lys, J and Lysak, R and Macqueen, D and Madrak, R and Maeshima, K and Makhoul, K and Maki, T and Maksimovic, P and Malde, S and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Marino, CP and Martin, A and Martin, V and Martínez, M and Martínez-Ballarín, R and Maruyama, T and Mastrandrea, P and Masubuchi, T and Mathis, M and Mattson, ME and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala,
P and Menzione, A and Merkel, P and Mesropian, C and Miao, T and Miladinovic, N and Miller, R and Mills, C and Milnik, M and Mitra, A and Mitselmakher, G and Miyake, H and Moggi, N and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mülmenstädt, J and Mukherjee, A and Muller, T and Mumford, R and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Nagano, A and Naganoma, J and Nakamura, K and Nakano, I and Napier, A and Necula, V and Nett, J and Neu, C and Neubauer, MS and Neubauer, S and Nielsen, J and Nodulman, L and Norman, M and Norniella, O and Nurse, E and Oakes, L and Oh, SH and Oh, YD and Oksuzian, I and Okusawa, T and Orava, R and Osterberg, K and Griso, SP and Palencia, E and Papadimitriou, V and Papaikonomou, A and Paramonov, AA and Parks, B and Pashapour, S and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Peiffer, T and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pinera, L and Pitts, K and Plager, C and Pondrom, L and Poukhov, O and Pounder, N and Prakoshyn, F and Pronko, A and Proudfoot, J and Ptohos,
F and Pueschel, E and Punzi, G and Pursley, J and Rademacker, J and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Renz, M and Rescigno, M and Richter, S and Rimondi, F and Ristori, L and Robson, A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Rossi, M and Rossin, R and Roy, P and Ruiz, A and Russ, J and Rusu, V and Rutherford, B and Saarikko, H and Safonov, A and Sakumoto,
WK and Saltó, O and Santi, L and Sarkar, S and Sartori, L and Sato, K and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schmidt, MA and Schmidt, MP and Schmitt, M and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Sedov, A and Seidel, S and Seiya, Y and Semenov, A and Sexton-Kennedy, L and Sforza, F and Sfyrla,
A and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shiraishi, S and Shochet, M and Shon, Y and Shreyber, I and Sidoti, A and Sinervo, P and Sisakyan, A and Slaughter, AJ and Slaunwhite, J and Sliwa, K and Smith, JR and Snider, FD and Snihur, R and Soha, A and Somalwar, S and Sorin, V and Spalding, J and Spreitzer, T and Squillacioti, P and Stanitzki, M and St Denis and R and Stelzer, B and Stelzer-Chilton, O and Stentz, D},
Title = {Search for the decays B_{(s)};{0} --> e;{+} micro;{-} and
B_{(s)};{0} --> e;{+} e;{-} in CDF run II.},
Journal = {Physical review letters},
Volume = {102},
Number = {20},
Pages = {201801},
Year = {2009},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.102.201801},
Abstract = {We report results from a search for the lepton flavor
violating decays B_{s};{0} --> e;{+} micro;{-} and B;{0} -->
e;{+} micro;{-}, and the flavor-changing neutral-current
decays B_{s};{0} --> e;{+} e;{-} and B;{0} --> e;{+} e;{-}.
The analysis uses data corresponding to 2 fb;{-1} of
integrated luminosity of pp[over ] collisions at sqrt[s] =
1.96 TeV collected with the upgraded Collider Detector (CDF
II) at the Fermilab Tevatron. The observed number of B0 and
B_{s};{0} candidates is consistent with background
expectations. The resulting Bayesian upper limits on the
branching ratios at 90% credibility level are B(B_{s};{0}
--> e;{+} micro;{-}) < 2.0 x 10;{-7}, B(B;{0} --> e;{+}
micro;{-}) < 6.4 x 10;{-8}, B(B_{s};{0} --> e;{+} e;{-}) <
2.8 x 10;{-7}, and B(B;{0} --> e;{+} e;{-}) < 8.3 x 10;{-8}.
From the limits on B(B_{(s)};{0} --> e;{+} micro;{-}), the
following lower bounds on the Pati-Salam leptoquark masses
are also derived: M_{LQ}(B_{s};{0} --> e;{+} micro;{-}) >
47.8 TeV/c;{2}, and M_{LQ}(B;{0} --> e;{+} micro;{-}) > 59.3
TeV / c;{2}, at 90% credibility level.},
Doi = {10.1103/physrevlett.102.201801},
Key = {fds307952}
}
@article{fds347488,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay,
NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines,
JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero,
M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann,
TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan,
P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheplakov,
A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Christodoulou, V and Chromek-Burckhart, D and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ},
Title = {Search for the Dimuon Decay of the Higgs Boson in pp
Collisions at sqrt[s]=13 TeV with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {119},
Number = {5},
Pages = {051802},
Year = {2017},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.119.051802},
Abstract = {A search for the dimuon decay of the Higgs boson was
performed using data corresponding to an integrated
luminosity of 36.1 fb^{-1} collected with the ATLAS
detector in pp collisions at sqrt[s]=13 TeV at the
Large Hadron Collider. No significant excess is observed
above the expected background. The observed (expected) upper
limit on the cross section times branching ratio is 3.0
(3.1) times the Standard Model prediction at the
95% confidence level for a Higgs boson mass of 125 GeV.
When combined with the pp collision data at
sqrt[s]=7 TeV and sqrt[s]=8 TeV, the observed
(expected) upper limit is 2.8 (2.9) times the Standard Model
prediction.},
Doi = {10.1103/physrevlett.119.051802},
Key = {fds347488}
}
@article{fds347468,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle,
P and Beck, HP and Beck, HC and Becker, K and Becker, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee,
CP and Beermann, TA and Begalli, M and Begel, M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz,
NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozson, AJ and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and Bruckman
de Renstrom, PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron,
J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou,
Y},
Title = {Search for the direct production of charginos and
neutralinos in final states with tau leptons in s = 13 TeV
pp collisions with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {78},
Number = {2},
Pages = {154},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-018-5583-9},
Abstract = {A search for the direct production of charginos and
neutralinos in final states with at least two hadronically
decaying tau leptons is presented. The analysis uses a
dataset of <i>pp</i> collisions corresponding to an
integrated luminosity of 36.1 fb - 1 , recorded with the
ATLAS detector at the Large Hadron Collider at a
centre-of-mass energy of 13 TeV. No significant deviation
from the expected Standard Model background is observed.
Limits are derived in scenarios of pair production and of
and production in simplified models where the neutralinos
and charginos decay solely via intermediate left-handed
staus and tau sneutrinos, and the mass of the τ ~ L state
is set to be halfway between the masses of the and the .
Chargino masses up to 630 GeV are excluded at 95% confidence
level in the scenario of direct production of for a massless
. Common and masses up to 760 GeV are excluded in the case
of production of and assuming a massless . Exclusion limits
for additional benchmark scenarios with large and small
mass-splitting between the and the are also studied by
varying the τ ~ L mass between the masses of the and the
.},
Doi = {10.1140/epjc/s10052-018-5583-9},
Key = {fds347468}
}
@article{fds313590,
Author = {The, ATLASC and Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J},
Title = {Search for the direct production of charginos, neutralinos
and staus in final states with at least two hadronically
decaying taus and missing transverse momentum in pp
collisions at √ $$ \sqrt{s}=8 $$ TeV with the ATLAS
detector},
Journal = {Critical Ultrasound Journal},
Volume = {2014},
Number = {10},
Year = {2014},
Month = {January},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP10(2014)096},
Abstract = {© 2014, The Author(s).Abstract: Results of a search for the
electroweak associated production of charginos and
next-to-lightest neutralinos, pairs of charginos or pairs of
tau sleptons are presented. These processes are
characterised by final states with at least two hadronically
decaying tau leptons, missing transverse momentum and low
jet activity. The analysis is based on an integrated
luminosity of 20.3 fb−1 of proton-proton collisions at
(Formula presented) recorded with the ATLAS experiment at
the Large Hadron Collider. No significant excess is observed
with respect to the predictions from Standard Model
processes. Limits are set at 95% confidence level on the
masses of the lighter chargino and next-to-lightest
neutralino for various hypotheses for the lightest
neutralino mass in simplified models. In the scenario of
direct production of chargino pairs, with each chargino
decaying into the lightest neutralino via an intermediate
tau slepton, chargino masses up to 345 GeV are excluded for
a massless lightest neutralino. For associated production of
mass-degenerate charginos and next-to-lightest neutralinos,
both decaying into the lightest neutralino via an
intermediate tau slepton, masses up to 410 GeV are excluded
for a massless lightest neutralino.[Figure not available:
see fulltext.]},
Doi = {10.1007/JHEP10(2014)096},
Key = {fds313590}
}
@article{fds356778,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for the electroweak production of supersymmetric
particles in √s = 8 TeV pp collisions with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {93},
Number = {5},
Year = {2016},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.93.052002},
Abstract = {The ATLAS experiment has performed extensive searches for
the electroweak production of charginos, neutralinos, and
staus. This article summarizes and extends the search for
electroweak supersymmetry with new analyses targeting
scenarios not covered by previously published searches. New
searches use vector-boson fusion production, initial-state
radiation jets, and low-momentum lepton final states, as
well as multivariate analysis techniques to improve the
sensitivity to scenarios with small mass splittings and
low-production cross sections. Results are based on 20 fb-1
of proton-proton collision data at √s = 8 TeV recorded
with the ATLAS experiment at the Large Hadron Collider. No
significant excess beyond Standard Model expectations is
observed. The new and existing searches are combined and
interpreted in terms of 95% confidence-level exclusion
limits in simplified models, where a single production
process and decay mode is assumed, as well as within
phenomenological supersymmetric models.},
Doi = {10.1103/PhysRevD.93.052002},
Key = {fds356778}
}
@article{fds356687,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze,
G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and d'Ascenzo,
N and Datta, M and de Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina,
K and Edgar, R and Elagin, A and Erbacher, R and Errede, S and Esham, B and Farrington, S and Fernández Ramos and JP and Field, R and Flanagan, G and Forrest, R and Franklin, M and Freeman, JC and Frisch, H and Funakoshi,
Y and Galloni, C and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gold, M and Goldin, D and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grosso-Pilcher, C and Guimaraes da Costa and J and Hahn, SR and Han, JY and Happacher, F and Hara, K and Hare, M and Harr, RF and Harrington-Taber,
T and Hatakeyama, K and Hays, C and Heinrich, J and Herndon, M and Hocker,
A and Hong, Z and Hopkins, W and Hou, S and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kambeitz, M and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kurata, M and Laasanen, AT and Lammel, S and Lancaster, M and Lannon, K and Latino, G and Lee, HS and Lee, JS and Leo,
S and Leone, S and Lewis, JD and Limosani, A and Lipeles, E and Lister, A and Liu, Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lucà,
A and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak,
R and Madrak, R and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Marchese, L and Margaroli, F and Marino,
P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Moon,
CS and Moore, R and Morello, MJ and Mukherjee, A and Muller, T and Murat,
P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano,
I and Napier, A and Nett, J and Nigmanov, T and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh, YD and Okusawa, T and Orava,
R and Ortolan, L and Pagliarone, C and Palencia, E and Palni, P and Papadimitriou, V and Parker, W and Pauletta, G and Paulini, M and Paus,
C and Phillips, TJ and Piacentino, G and Pianori, E and Pilot, J and Pitts,
K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Pranko, A and Prokoshin, F and Ptohos, F and Punzi, G and Redondo
Fernández, I and Renton, P and Rescigno, M and Rimondi, F and Ristori,
L and Robson, A and Rodriguez, T and Rolli, S and Ronzani, M and Roser, R and Rosner, JL and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, EE and Schwarz, T and Scodellaro, L and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima,
M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sliwa, K and Smith, JR and Snider, FD and Song, H and Sorin, V and St Denis and R and Stancari, M and Stentz, D and Strologas, J and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thomson, E and Thukral, V and Toback, D and Tokar,
S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta,
D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Vázquez,
F and Velev, G and Vellidis, C and Vernieri, C and Vidal, M and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wallny, R and Wang,
SM and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wilbur, S and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfmeister, H and Wright, T and Wu, X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang, YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu,
GB and Yu, I and Zanetti, AM and Zeng, Y and Zhou, C and Zucchelli, S and CDF
Collaboration},
Title = {Search for the Exotic Meson X(5568) with the Collider
Detector at Fermilab.},
Journal = {Physical review letters},
Volume = {120},
Number = {20},
Pages = {202006},
Year = {2018},
Month = {May},
url = {http://dx.doi.org/10.1103/physrevlett.120.202006},
Abstract = {A search for the exotic meson X(5568) decaying into the
B_{s}^{0}π^{±} final state is performed using data
corresponding to 9.6 fb^{-1} from pp[over ¯]
collisions at sqrt[s]=1960 GeV recorded by the Collider
Detector at Fermilab. No evidence for this state is found
and an upper limit of 6.7% at the 95% confidence level is
set on the fraction of B_{s}^{0} produced through the
X(5568)→B_{s}^{0}π^{±} process.},
Doi = {10.1103/physrevlett.120.202006},
Key = {fds356687}
}
@article{fds308006,
Author = {Collaboration, DAEACDF},
Title = {Search for the flavor-changing neutral current decay
D0-->µ+µ- in pp-bar collisions at sqrt[s]=1.96 TeV},
Journal = {Physical Review},
Volume = {D68},
Number = {19},
Pages = {091101},
Year = {2003},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevlett.101.192002},
Abstract = {We report on a search for the flavor-changing neutral
current decay D0-->µ+µ- in pp-bar collisions at
sqrt[s]=1.96 TeV using 65 pb-1 of data collected by the
CDF II experiment at the Fermilab Tevatron Collider. A
displaced-track trigger selects long-lived D0 candidates in
the D0-->µ+µ- search channel, the kinematically similar
D0--> pi + pi - channel used for normalization, the
Cabibbo-favored D0-->K- pi + channel used to optimize the
selection criteria in an unbiased manner, and their charge
conjugates. Finding no signal events in the D0-->µ+µ-
search window, we set an upper limit on the branching
fractionB(D0-- >µ+µ-)},
Doi = {10.1103/physrevlett.101.192002},
Key = {fds308006}
}
@article{fds351089,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G},
Title = {Search for the HH → bb¯ bb¯ process via vector-boson
fusion production using proton-proton collisions at √s =
13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {7},
Year = {2020},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2020)108},
Abstract = {A search for Higgs boson pair production via vector-boson
fusion (VBF) in the bb¯ bb¯ final state is carried out
with the ATLAS experiment using 126 fb−1 of proton- proton
collision data delivered at s = 13 TeV by the Large Hadron
Collider. This search is sensitive to VBF production of
additional heavy bosons that may decay into Higgs boson
pairs, and in a non-resonant topology it can constrain the
quartic coupling between the Higgs bosons and vector bosons.
No significant excess relative to the Standard Model
expectation is observed, and limits on the production
cross-section are set at the 95% confidence level for a
heavy scalar resonance in the context of an extended Higgs
sector, and for non-resonant Higgs boson pair production.
Interpretation in terms of the coupling between a Higgs
boson pair and two vector bosons is also provided: coupling
values normalised to the Standard Model expectation of κ2V<
−0.76 and κ2V> 2.90 are excluded at the 95% confidence
level in data. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP07(2020)108},
Key = {fds351089}
}
@article{fds356541,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Search for the Higgs boson decays H → ee and
H → eμ in pp collisions at s=13TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {801},
Year = {2020},
Month = {February},
url = {http://dx.doi.org/10.1016/j.physletb.2019.135148},
Abstract = {Searches for the Higgs boson decays H→ee and H→eμ are
performed using data corresponding to an integrated
luminosity of 139fb−1 collected with the ATLAS detector in
pp collisions at s=13 TeV at the LHC. No significant signals
are observed, in agreement with the Standard Model
expectation. For a Higgs boson mass of 125 GeV, the observed
(expected) upper limit at the 95% confidence level on the
branching fraction B(H→ee) is 3.6×10−4 (3.5×10−4)
and on B(H→eμ) is 6.2×10−5 (5.9×10−5). These
results represent improvements by factors of about five and
six on the previous best limits on B(H→ee) and B(H→eμ)
respectively.},
Doi = {10.1016/j.physletb.2019.135148},
Key = {fds356541}
}
@article{fds307688,
Author = {Aaltonen, T and González, BA and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De Barbaro and P and Dell'orso, M and Demortier, L and Deninno, M and Devoto, F},
Title = {Search for the Higgs boson in the all-hadronic final state
using the full CDF data set},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {2},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP02(2013)004},
Abstract = {This paper reports the result of a search for the standard
model Higgs boson in events containing four reconstructed
jets associated with quarks. For masses below 135 GeV/c 2,
the Higgs boson decays to bottom-antibottom quark pairs are
dominant and result primarily in two hadronic jets. An
additional two jets can be produced in the hadronic decay of
a W or Z boson produced in association with the Higgs boson,
or from the incoming quarks that produced the Higgs boson
through the vector-boson fusion process. The search is
performed using a sample of √s=1.96 TeV proton-antiproton
collisions corresponding to an integrated luminosity of 9.45
fb-1 recorded by the CDF II detector. The data are in
agreement with the background model and 95% credibility
level upper limits on Higgs boson production are set as a
function of the Higgs boson mass. The median expected
(observed) limit for a 125 GeV/c 2 Higgs boson is 11.0 (9.0)
times the predicted standard model rate. © 2013
SISSA.},
Doi = {10.1007/JHEP02(2013)004},
Key = {fds307688}
}
@article{fds307740,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten,
K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa,
HS and Beale, S and Beare, B and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks,
KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde,
M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos,
N and Benhammou, Y and Benitez Garcia and JA and Benjamin, DP and Benoit,
M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth,
JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba,
LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana,
S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero,
J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Caramarcu, C and Cardarelli,
R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens,
JC and Clement, B and Clement, C},
Title = {Search for the Higgs boson in the H→WW(*)→ℓ(+)νℓ(-)ν
decay channel in pp collisions at √s=7 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {108},
Number = {11},
Pages = {111802},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.108.111802},
Abstract = {A search for the Higgs boson has been performed in the
H→WW(*)→ℓ(+)νℓ(-)ν[over ¯] channel (ℓ=e/μ)
with an integrated luminosity of 2.05 fb(-1) of pp
collisions at √s=7 TeV collected with the ATLAS detector
at the Large Hadron Collider. No significant excess of
events over the expected background is observed and limits
on the Higgs boson production cross section are derived for
a Higgs boson mass in the range 110 GeV<m(H)<300 GeV. The
observations exclude the presence of a standard model Higgs
boson with a mass 145<m(H)<206 GeV at 95% confidence
level.},
Doi = {10.1103/physrevlett.108.111802},
Key = {fds307740}
}
@article{fds307830,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Atoian, G and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Austin, N and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos,
G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Bachy, G and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro
Galtieri, A and Barber, T and Barberio, EL and Barberis, D and Barbero,
M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett, RM and Baroncelli, A and Barone,
G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, D and Bartsch,
V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Battistoni, G and Bauer, F and Bawa, HS and Beare, B and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian,
S and Bednyakov, VA and Bee, CP and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Ben Ami and S and Benary, O and Benchekroun, D and Benchouk, C and Bendel,
M and Benekos, N and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernardet, K and Bernat, P and Bernhard, R and Bernius,
C and Berry, T and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada,
J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Böser, S and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Boorman, G and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borroni, S and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Breton, D and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Brooijmans, G and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet,
S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Buira-Clark, D and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byatt, T and Cabrera
Urbán, S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio,
A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan,
K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari,
G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciba, K and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC and Clement, B and Clement, C and Clifft, RW and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coe, P and Cogan, JG},
Title = {Search for the Higgs boson in the H→WW→lνjj decay
channel in pp collisions at √s=7 TeV with the ATLAS
detector.},
Journal = {Physical review letters},
Volume = {107},
Number = {23},
Pages = {231801},
Year = {2011},
Month = {December},
url = {http://dx.doi.org/10.1103/physrevlett.107.231801},
Abstract = {A search for a Higgs boson has been performed in the
H→WW→ℓνjj channel in 1.04 fb(-1) of pp collision data
at √s=7 TeV recorded with the ATLAS detector at the Large
Hadron Collider. No significant excess of events is observed
over the expected background and limits on the Higgs boson
production cross section are derived for a Higgs boson mass
in the range 240 GeV<m(H)<600 GeV. The best sensitivity is
reached for m(H)=400 GeV, where the 95% confidence level
upper bound on the cross section for H→WW production is
3.1 pb, or 2.7 times the standard model prediction.},
Doi = {10.1103/physrevlett.107.231801},
Key = {fds307830}
}
@article{fds307656,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for the Higgs boson in the H→WW→ℓνjj decay
channel at √s=7 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {718},
Number = {2},
Pages = {391-410},
Publisher = {Elsevier BV},
Year = {2012},
Month = {December},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.10.066},
Abstract = {A search for the Standard Model Higgs boson has been
performed in the H→WW→ℓνjj channel using 4.7 fb−1
of pp collision data recorded at a centre-of-mass energy of
s=7 TeV with the ATLAS detector at the Large Hadron
Collider. Higgs boson candidates produced in association
with zero, one or two jets are included in the analysis to
maximize the acceptance for both gluon fusion and weak boson
fusion Higgs boson production processes. No significant
excess of events is observed over the expected background
and limits on the Higgs boson production cross section are
derived for a Higgs boson mass in the range 300 GeV<mH<600
GeV. The best sensitivity is reached for mH=400 GeV, where
the observed (expected) 95% confidence level upper bound on
the cross section for H→WW produced in association with
zero or one jet is 2.2 pb (1.9 pb), corresponding to 1.9
(1.6) times the Standard Model prediction. In the Higgs
boson plus two jets channel, which is more sensitive to the
weak boson fusion process, the observed (expected) 95%
confidence level upper bound on the cross section for H→WW
production with mH=400 GeV is 0.7 pb (0.6 pb), corresponding
to 7.9 (6.5) times the Standard Model prediction.},
Doi = {10.1016/j.physletb.2012.10.066},
Key = {fds307656}
}
@article{fds356654,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Search for the Higgs boson produced in association with a
vector boson and decaying into two spin-zero particles in
the H → aa → 4b channel in pp collisions at √s=13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {10},
Year = {2018},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2018)031},
Abstract = {A search for exotic decays of the Higgs boson into a pair of
spin-zero particles, H → aa, where the a-boson decay sin
to b-quarks promptly or with a mean proper lifetime cτa up
to 6 mm and has a mass in the range of 20–60 GeV, is
presented. The search is performed in events where the Higgs
boson is produced in association with a W or Z boson, giving
rise to a signature of one or two charged leptons (electrons
or muons) and multiple jets from b-quark decays. The
analysis is based on the dataset of proton-proton collisions
at s=13 TeV recorded in 2015 and 2016 by the ATLAS detector
at the CERN Large Hadron Collider, corresponding to an
integrated luminosity of 36.1 fb−1. No significant excess
of events above the Standard Model background prediction is
observed, and 95% confidence-level upper limits are derived
for the production cross-sections for pp → WH, ZH and
their combination, times the branching ratio of the decay
chain H → aa → 4b. For a-bosons which decay promptly,
the upper limit on the combination of cross-sections for WH
and ZH times the branching ratio of H → aa → 4b ranges
from 3.0 pb for ma = 20 GeV to 1.3 pb for ma = 60 GeV,
assuming that the ratio of WH to ZH cross-sections follows
the Standard Model prediction. For a-bosons with longer
proper lifetimes, the most stringent limits are 1.8 pb and
0.68 pb, respectively, at cτa ∼ 0.4 mm.[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP10(2018)031},
Key = {fds356654}
}
@article{fds323242,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz,
NV and Biglietti, M and De Mendizabal and JB and Billoud, TRV and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Lopez, SC and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli,
A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich,
LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti,
F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen,
X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A},
Title = {Search for the Higgs boson produced in association with a W
boson and decaying to four b-quarks via two spin-zero
particles in pp collisions at 13 TeV with the ATLAS
detector.},
Journal = {Eur Phys J C Part Fields},
Volume = {76},
Number = {11},
Pages = {605},
Year = {2016},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4418-9},
Abstract = {This paper presents a dedicated search for exotic decays of
the Higgs boson to a pair of new spin-zero particles,
[Formula: see text], where the particle a decays to b-quarks
and has a mass in the range of 20-60 GeV. The search is
performed in events where the Higgs boson is produced in
association with a [Formula: see text] boson, giving rise to
a signature of a lepton (electron or muon), missing
transverse momentum, and multiple jets from b-quark decays.
The analysis is based on the full dataset of pp collisions
at [Formula: see text] recorded in 2015 by the ATLAS
detector at the CERN Large Hadron Collider, corresponding to
an integrated luminosity of 3.2 [Formula: see text]. No
significant excess of events above the Standard Model
prediction is observed, and a [Formula: see text]
confidence-level upper limit is derived for the product of
the production cross section for [Formula: see text] times
the branching ratio for the decay [Formula: see text]. The
upper limit ranges from 6.2 pb for an a-boson mass
[Formula: see text] to 1.5 pb for [Formula: see
text].},
Doi = {10.1140/epjc/s10052-016-4418-9},
Key = {fds323242}
}
@article{fds308004,
Author = {Aaltonen, T and others},
Title = {Search for the Higgs Boson Produced in Association with
Z→ℓ+ℓ- in pp̅ Collisions at sqrt[s] =1.96
TeV},
Journal = {Physical Review Letters},
Volume = {101},
Number = {25},
Pages = {251803},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.251803},
Abstract = {We present a search for the Higgs boson in the process qq̅
→ZH→ℓ+ℓ-bb̅ . The analysis uses an integrated
luminosity of 1 fb-1 of pp̅ collisions produced at
sqrt[s]=1.96 TeV and accumulated by the upgraded
Collider Detector at Fermilab (CDF II). We employ artificial
neural networks both to correct jets mismeasured in the
calorimeter and to distinguish the signal kinematic
distributions from those of the background. We see no
evidence for Higgs boson production, and set 95% C.L. upper
limits on σZHB(H→bb̅ ), ranging from 1.5 to 1.2 pb for a
Higgs boson mass (mH) of 110 to 150 GeV/c2.},
Doi = {10.1103/physrevlett.101.251803},
Key = {fds308004}
}
@article{fds307992,
Author = {Aaltonen, T and others},
Title = {Search for the Higgs boson produced in association with
Z→ℓ+ℓ- using the matrix element method at CDF
II},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {7},
Pages = {071101},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.071101},
Abstract = {We present a search for associated production of the
standard model Higgs boson and a Z boson where the Z boson
decays to two leptons and the Higgs decays to a pair of b
quarks in pp̅ collisions at the Fermilab Tevatron. We use
event probabilities based on standard model matrix elements
to construct a likelihood function of the Higgs content of
the data sample. In a CDF data sample corresponding to an
integrated luminosity of 2.7 fb-1 we see no evidence of
a Higgs boson with a mass between 100 GeV/c2 and
150 GeV/c2. We set 95% confidence level upper limits on
the cross section for ZH production as a function of the
Higgs boson mass mH; the limit is 8.2 times the standard
model prediction at mH=115 GeV/c2.},
Doi = {10.1103/PhysRevD.80.071101},
Key = {fds307992}
}
@article{fds310354,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Djuvsland, JI and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Kucuk, H and Anisenkov,
AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Search for the lepton flavor violating decay Z → eμ in pp
collisions at √s = 8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.90.072010},
Abstract = {The ATLAS detector at the Large Hadron Collider is used to
search for the lepton flavor violating process Z → eμ in
pp collisions using 20.3 fb-1 of data collected at √s = 8
TeV. An enhancement in the eμ invariant mass spectrum is
searched for at the Z-boson mass. The number of Z bosons
produced in the data sample is estimated using events of
similar topology, Z → ee and μμ, significantly reducing
the systematic uncertainty in the measurement. There is no
evidence of an enhancement at the Z-boson mass, resulting in
an upper limit on the branching fraction, B(Z → 7.5 ×
10.7 at the 95% confidence level.},
Doi = {10.1103/PhysRevD.90.072010},
Key = {fds310354}
}
@article{fds307977,
Author = {Aaltonen, T and others},
Title = {Search for the neutral current top quark decay t→Zc using
the ratio of Z-boson+4 jets to W-boson+4 jets
production},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {5},
Pages = {052001},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.052001},
Abstract = {We have used the Collider Detector at Fermilab (CDF-II) to
search for the flavor-changing neutral-current (FCNC)
top-quark decay t→Zc using a technique employing ratios of
W and Z production, measured in pp̅ data corresponding to
an integrated luminosity of 1.52 fb-1. The analysis
uses a comparison of two decay chains, pp̅ →tt̅
→WbWb→ℓνbjjb and pp̅ →tt̅ →ZcWb→ℓℓcjjb,
to cancel systematic uncertainties in acceptance,
efficiency, and luminosity. We validate the modeling of
acceptance and efficiency for lepton identification over the
multiyear data set using another ratio of W and Z
production, in this case the observed ratio of inclusive
production of W to Z bosons. To improve the discrimination
against standard model backgrounds to top-quark decays, we
calculate the top-quark mass for each event with two leptons
and four jets assuming it is a tt̅ event with one of the
top quarks decaying to Zc. For additional background
discrimination we require at least one jet to be identified
as originating from a b quark. No significant signal is
found and we set an upper limit on the FCNC branching ratio
Br(t→Zc) using a likelihood constructed from the
ℓℓcjjb top-quark mass distribution and the number of
ℓνbjjb events. Limits are set as a function of the
helicity of the Z boson produced in the FCNC decay. For 100%
longitudinally-polarized Z bosons we find limits of 8.3% and
9.3% (95% C.L.) depending on the assumptions regarding the
theoretical top-quark pair production cross
section.},
Doi = {10.1103/PhysRevD.80.052001},
Key = {fds307977}
}
@article{fds307630,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E},
Title = {Search for the neutral Higgs bosons of the minimal
supersymmetric standard model in pp collisions at √s = 7
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {2},
Pages = {1-46},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP02(2013)095},
Abstract = {A search for neutral Higgs bosons of the Minimal
Supersymmetric Standard Model (MSSM) is reported. The
analysis is based on a sample of proton-proton collisions at
a centre-of-mass energy of 7TeV recorded with the ATLAS
detector at the Large Hadron Collider. The data were
recorded in 2011 and correspond to an integrated luminosity
of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into
oppositely-charged muon or τ lepton pairs are considered
for final states requiring either the presence or absence of
b-jets. No statistically significant excess over the
expected background is observed and exclusion limits at the
95% confidence level are derived. The exclusion limits are
for the production cross-section of a generic neutral Higgs
boson, φ, as a function of the Higgs boson mass and for
h/A/H production in the MSSM as a function of the parameters
mA and tan β in the mhmax scenario for mA in the range of
90GeV to 500 GeV. Copyright CERN.},
Doi = {10.1007/JHEP02(2013)095},
Key = {fds307630}
}
@article{fds347444,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Armitage, LJ and Armstrong, A and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Asimakopoulou, EM and Asquith, L and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Avramidou, R and Ayoub, MK and Azoulay, AM and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Bailey, AJ and Bailey, VR and Baines,
JT and Bajic, M and Bakalis, C and Baker, OK and Bakker, PJ and Bakshi
Gupta, D and Balaji, S and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Balz, J and Banas, E and Bandyopadhyay, A and Banerjee,
S and Bannoura, AAE and Barak, L and Barbe, WM and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnea, R and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone,
G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batlamous,
S and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bauer, KT and Bawa, HS and Beacham, JB and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HC and Beck, HP and Becker, K and Becker, M and Becot, C and Beddall,
A and Beddall, AJ and Bednyakov, VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beisiegel, F and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellomo, M and Bellos, P and Belotskiy, K and Belyaev, NL and Benary,
O and Benchekroun, D and Bender, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Bergsten, LJ and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertram, IA and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Bethani, A and Bethke, S and Betti, A and Bevan, AJ and Beyer, J and Bi, R and Bianchi,
RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Birman, M and Bisanz, T and Biswal, JP and Bittrich, C and Bjergaard, DM and Black, JE and Black, KM and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert,
V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Bonilla, JS and Boonekamp, M and Borecka-Bielska, HM and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bozson, AJ and Bracinik, J and Brahimi, N and Brandt, A and Brandt, G and Brandt, O and Braren, F and Bratzler, U and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brenner, L and Brenner,
R and Bressler, S and Brickwedde, B and Briglin, DL and Britton, D and Britzger, D and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brost, E and Broughton, JH and Bruckman de Renstrom,
PA and Bruncko, D and Bruni, A and Bruni, G and Bruni, LS and Bruno, S and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov,
IA and Bugge, MK and Bührer, F and Bulekov, O and Bullock, D and Burch,
TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Büscher, V and Buschmann, E and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai,
H and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Cao, Y and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, FC and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carter, JWS and Casadei, D and Casado, MP and Casha,
AF and Casper, DW and Castelijn, R and Castillo, FL and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty,
D and Chan, SK and Chan, WS and Chapman, JD and Chargeishvili, B and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, CH and Chen, H and Chen, J and Chen,
S and Chen, SJ and Chen, X and Chen, Y and Chen, Y-H and Cheng, HC and Cheng,
HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalérias, TJA and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, I and Chiu, YH and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S},
Title = {Search for the Production of a Long-Lived Neutral Particle
Decaying within the ATLAS Hadronic Calorimeter in
Association with a Z Boson from pp Collisions at
sqrt[s]=13 TeV.},
Journal = {Physical review letters},
Volume = {122},
Number = {15},
Pages = {151801},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.122.151801},
Abstract = {This Letter presents a search for the production of a
long-lived neutral particle (Z_{d}) decaying within the
ATLAS hadronic calorimeter, in association with a standard
model (SM) Z boson produced via an intermediate scalar
boson, where Z→ℓ^{+}ℓ^{-} (ℓ=e, μ). The data used
were collected by the ATLAS detector during 2015 and 2016 pp
collisions with a center-of-mass energy of
sqrt[s]=13 TeV at the Large Hadron Collider and
correspond to an integrated luminosity of
36.1±0.8 fb^{-1}. No significant excess of events is
observed above the expected background. Limits on the
production cross section of the scalar boson times its decay
branching fraction into the long-lived neutral particle are
derived as a function of the mass of the intermediate scalar
boson, the mass of the long-lived neutral particle, and its
cτ from a few centimeters to one hundred meters. In the
case that the intermediate scalar boson is the SM Higgs
boson, its decay branching fraction to a long-lived neutral
particle with a cτ approximately between 0.1 and 7 m is
excluded with a 95% confidence level up to 10% for
m_{Z_{d}} between 5 and 15 GeV.},
Doi = {10.1103/physrevlett.122.151801},
Key = {fds347444}
}
@article{fds307947,
Author = {Aaltonen, T and others},
Title = {Search for the Production of Narrow tb̅ Resonances in 1.9
fb-1 of pp̅ Collisions at sqrt[s] =1.96
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {103},
Number = {4},
Pages = {041801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.103.041801},
Abstract = {We present new limits on resonant tb̅ production in pp̅
collisions at sqrt[s]=1.96 TeV, using 1.9 fb-1 of
data recorded with the CDF II detector at the Fermilab
Tevatron. We reconstruct a candidate tb̅ mass in events
with a lepton, neutrino candidate, and two or three jets,
and search for anomalous tb̅ production as modeled by
W′→tb̅ . We set a new limit on a right-handed W′ with
standard model-like coupling, excluding any mass below
800 GeV/c2 at 95% C.L. The cross section for any
narrow, resonant tb̅ production between 750 and
950 GeV/c2 is found to be less than 0.28 pb at 95% C.L.
We also present an exclusion of the W′ coupling strength
versus W′ mass over the range 300--950 GeV/c2.},
Doi = {10.1103/physrevlett.103.041801},
Key = {fds307947}
}
@article{fds307899,
Author = {Aaltonen, and T, and others},
Title = {Search for the Production of Scalar Bottom Quarks in $p
\bar{p}$ collisions at $\sqrt{s} = 1.96$
TeV},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {8},
Pages = {081802},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.081802},
Abstract = {http://arxiv.org/abs/1005.3600},
Doi = {10.1103/PhysRevLett.105.081802},
Key = {fds307899}
}
@article{fds314797,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for the production of single vector-like and excited
quarks in the Wt final state in pp collisions at √s = 8
TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {2},
Pages = {1-46},
Publisher = {Springer Nature},
Year = {2016},
Month = {February},
url = {http://dx.doi.org/10.1007/JHEP02(2016)110},
Abstract = {A search for vector-like quarks and excited quarks in events
containing a top quark and a W boson in the final state is
reported here. The search is based on 20.3 fb−1 of
proton-proton collision data taken at the LHC at a
centre-of-mass energy of 8 TeV recorded by the ATLAS
detector. Events with one or two leptons, and one, two or
three jets are selected with the additional requirement that
at least one jet contains a b-quark. Single-lepton events
are also required to contain at least one large-radius jet
from the hadronic decay of a high-pTW boson or a top quark.
No significant excess over the expected background is
observed and upper limits on the cross-section times
branching ratio for different vector-like quark and
excited-quark model masses are derived. For the
excited-quark production and decay to Wt with unit
couplings, quarks with masses below 1500 GeV are excluded
and coupling-dependent limits are set.},
Doi = {10.1007/JHEP02(2016)110},
Key = {fds314797}
}
@article{fds307562,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Search for the production of ZW and ZZ boson pairs decaying
into charged leptons and jets in pp̄ collisions at
√s=1.96 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {9},
Pages = {092002},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.88.092002},
Abstract = {We present a measurement of the production cross section for
ZW and ZZ boson pairs in final states with a pair of charged
leptons, from the decay of a Z boson, and at least two jets,
from the decay of a W or Z boson, using the full sample of
proton-antiproton collisions recorded with the CDF II
detector at the Tevatron, corresponding to 8.9 fb-1 of
integrated luminosity. We increase the sensitivity to
vector-boson decays into pairs of quarks using a
neural-network discriminant that exploits the differences
between the spatial spread of energy depositions and
charged-particle momenta contained within the jet of
particles originating from quarks and gluons. Additionally,
we employ new jet energy corrections to Monte Carlo
simulations that account for differences in the observed
energy scales for quark and gluon jets. The number of signal
events is extracted through a simultaneous fit to the dijet
mass spectrum in three classes of events: events likely to
contain jets with a heavy-quark decay, events likely to
contain jets originating from light quarks, and events that
fail these identification criteria. We determine the
production cross section to be σZW+ZZ=2.5-1.0+2.0 pb (<6.1
pb at the 95% confidence level), consistent with the
standard model prediction of 5.1 pb. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.88.092002},
Key = {fds307562}
}
@article{fds307969,
Author = {Aaltonen, T and Adelman, J and Akimoto, T and Albrow, MG and Álvarez
González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi,
A and Antos, J and Apollinari, G and Apresyan, A and Arisawa, T and Artikov, A and Ashmanskas, W and Attal, A and Aurisano, A and Azfar, F and Azzurri, P and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Bartsch, V and Bauer, G and Beauchemin, PH and Bedeschi,
F and Bednar, P and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beringer, J and Bhatti,
A and Binkley, M and Bisello, D and Bizjak, I and Blair, RE and Blocker, C and Blumenfeld, B and Bocci, A and Bodek, A and Boisvert, V and Bolla, G and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Bridgeman,
A and Brigliadori, L and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Byrum, KL and Cabrera, S and Calancha, C and Campanelli,
M and Campbell, M and Canelli, F and Canepa, A and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chang, SH and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli,
D and Chou, JP and Choudalakis, G and Chuang, SH and Chung, K and Chung,
WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clark, D and Compostella, G},
Title = {Search for the rare decays B+→μ+μ-K+, B0→μ+μ-
K*(892)0, and Bs0→μ+μ- at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {79},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.79.011104},
Abstract = {We search for b→sμ+μ- transitions in B meson (B+, B0, or
Bs0) decays with 924pb-1 of pp̄ collisions at s=1.96TeV
collected with the CDF II detector at the Fermilab Tevatron.
We find excesses with significances of 4.5, 2.9, and 2.4
standard deviations in the B+→μ+μ-K+,
B0→μ+μ-K*(892)0, and Bs0→μ+μ- decay modes,
respectively. Using B→J/ψh (h=K+, K*(892)0,) decays as
normalization channels, we report branching fractions for
the previously observed B+ and B0 decays,
B(B+→μ+μ-K+)=(0.59±0.15±0. 04)×10-6, and
B(B0→μ+μ-K*(892)0)=(0.81±0. 30±0.10)×10-6, where the
first uncertainty is statistical, and the second is
systematic. We set an upper limit on the relative branching
fraction B(Bs0→μ+μ-)/B(Bs0→J/ψ)<2.6(2.3)×10-3 at the
95(90)% confidence level, which is the most stringent to
date. © 2009 The American Physical Society.},
Doi = {10.1103/PhysRevD.79.011104},
Key = {fds307969}
}
@article{fds307805,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brau, B and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar and C and Cuevas, J and Culbertson, R},
Title = {Search for the rare radiative decay W→πγ in pp̄
collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.85.032001},
Abstract = {We present a search for the rare radiative decay W ±→ π
±γ using data corresponding to an integrated luminosity of
4.3fb -1 of proton-antiproton collisions at a center-of-mass
energy of 1.96 TeV collected by the CDF experiment at
Fermilab. As no statistically significant signal is
observed, we set a 95%-confidence-level upper limit on the
relative branching fraction Γ(W ±→π ±γ)/Γ(W ±→e
±ν) at 6.4×10 -5, a factor of 10 improvement over the
previous limit. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.85.032001},
Key = {fds307805}
}
@article{fds308175,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Baldin,
B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto,
J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette,
F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and de Jong, SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV and Duensing, S and Duflot, L and Dugad, SR},
Title = {Search for the Scalar Top Quark in [Formula presented]
Collisions at [Formula presented]},
Journal = {Physical Review Letters},
Volume = {88},
Number = {17},
Pages = {6},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.88.171802},
Abstract = {We have performed a search for scalar top quark (stop) pair
production in the inclusive electron-muon-missing transverse
energy final state, using a sample of [Formula presented]
events corresponding to [Formula presented] of data
collected with the D0 detector at Fermilab. The search is
done in the framework of the minimal supersymmetric standard
model assuming that the sneutrino is the lightest
supersymmetric particle. For the dominant decays of the
lightest stop, [Formula presented] and [Formula presented],
no evidence for signal is found. We derive cross-section
limits as a function of stop ([Formula presented]), chargino
([Formula presented]), and sneutrino ([Formula presented])
masses. © 2002 The American Physical Society.},
Doi = {10.1103/PhysRevLett.88.171802},
Key = {fds308175}
}
@article{fds310382,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for the Standard Model Higgs boson decay to
μ+μ− with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {738},
Number = {1},
Pages = {68-86},
Publisher = {Elsevier BV},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2014.09.008},
Abstract = {A search is reported for Higgs boson decay to μ+μ− using
data with an integrated luminosity of 24.8 fb−1collected
with the ATLAS detector in pp collisions at s=7and8 TeV at
the CERN Large Hadron Collider. The observed dimuon
invariant mass distribution is consistent with the Standard
Model background-only hypothesis in the 120–150 GeV search
range. For a Higgs boson with a mass of 125.5 GeV, the
observed (expected) upper limit at the 95% confidence level
is 7.0 (7.2) times the Standard Model expectation. This
corresponds to an upper limit on the branching ratio
BR(H→μ+μ−) of 1.5×10−3.},
Doi = {10.1016/j.physletb.2014.09.008},
Key = {fds310382}
}
@article{fds317296,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Search for the Standard Model Higgs boson decaying into bb¯
produced in association with top quarks decaying
hadronically in pp collisions at √s = 8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {5},
Publisher = {Springer Nature},
Year = {2016},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2016)160},
Abstract = {A search for Higgs boson production in association with a
pair of top quarks (tt¯ H) is performed, where the Higgs
boson decays to bb¯, and both top quarks decay
hadronically. The data used correspond to an integrated
luminosity of 20.3 fb−1 of pp collisions at √s = 8 TeV
collected with the ATLAS detector at the Large Hadron
Collider. The search selects events with at least six
energetic jets and uses a boosted decision tree algorithm to
discriminate between signal and Standard Model background.
The dominant multijet background is estimated using a
dedicated data-driven technique. For a Higgs boson mass of
125 GeV, an upper limit of 6.4 (5.4) times the Standard
Model cross section is observed (expected) at 95% confidence
level. The best-fit value for the signal strength is μ =
1.6 ± 2.6 times the Standard Model expectation for mH = 125
GeV. Combining all tt¯ H searches carried out by ATLAS at
√s = 8 and 7 TeV, an observed (expected) upper limit of
3.1 (1.4) times the Standard Model expectation is obtained
at 95% confidence level, with a signal strength μ = 1.7 ±
0.8.},
Doi = {10.1007/JHEP05(2016)160},
Key = {fds317296}
}
@article{fds307686,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley,
ME and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci,
A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba,
A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery,
ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and d'Ascenzo, N and Datta, M and de Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto, F and d'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dong,
P and Dorigo, M and Dorigo, T and Ebina, K and Elagin, A and Eppig, A and Erbacher, R and Errede, S and Ershaidat, N and Eusebi, R and Farrington,
S and Feindt, M and Fernandez, JP and Field, R and Flanagan, G and Forrest,
R and Frank, MJ and Franklin, M and Freeman, JC and Funakoshi, Y and Furic,
I and Gallinaro, M and Garcia, JE and Garfinkel, AF and Garosi, P and Gerberich, H and Gerchtein, E and Giagu, S and Giakoumopoulou, V and Giannetti, P and Gibson, K and Ginsburg, CM and Giokaris, N and Giromini, P and Giurgiu, G and Glagolev, V and Glenzinski, D and Gold,
M and Goldin, D and Goldschmidt, N and Golossanov, A and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González, O and Gorelov, I and Goshaw, AT and Goulianos, K and Grinstein, S and Grosso-Pilcher, C and Group, RC and Guimaraes da Costa and J and Hahn, SR and Halkiadakis, E and Hamaguchi, A and Han, JY and Happacher, F and Hara, K and Hare, D and Hare,
M and Harr, RF and Hatakeyama, K and Hays, C and Heck, M and Heinrich, J and Herndon, M and Hewamanage, S and Hocker, A and Hopkins, W and Horn, D and Hou, S and Hughes, RE and Hurwitz, M and Husemann, U and Hussain, N and Hussein, M and Huston, J and Introzzi, G and Iori, M and Ivanov, A and James, E and Jang, D and Jayatilaka, B and Jeon, EJ and Jindariani, S and Jones, M and Joo, KK and Jun, SY and Junk, TR and Kamon, T and Karchin, PE and Kasmi, A and Kato, Y and Ketchum, W and Keung, J and Khotilovich, V and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SB and Kim, SH and Kim, YK and Kim, YJ and Kimura, N and Kirby, M and Klimenko, S and Knoepfel, K and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kreps, M and Kroll, J and Krop, D and Kruse, M and Krutelyov, V and Kuhr,
T and Kurata, M and Kwang, S and Laasanen, AT and Lami, S and Lammel, S and Lancaster, M and Lander, RL and Lannon, K and Lath, A and Latino, G and LeCompte, T and Lee, E and Lee, HS and Lee, JS and Lee, SW and Leo, S and Leone, S and Lewis, JD and Limosani, A and Lin, C-J and Lindgren, M and Lipeles, E and Lister, A and Litvintsev, DO and Liu, C and Liu, H and Liu,
Q and Liu, T and Lockwitz, S and Loginov, A and Lucchesi, D and Lueck, J and Lujan, P and Lukens, P and Lungu, G and Lys, J and Lysak, R and Madrak, R and Maeshima, K and Maestro, P and Malik, S and Manca, G and Manousakis-Katsikakis, A and Margaroli, F and Marino, C and Martínez, M and Mastrandrea, P and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McFarland, KS and McIntyre, P and McNulty, R and Mehta, A and Mehtala, P and Mesropian, C and Miao, T and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondragon, MN and Moon, CS and Moore, R and Morello, MJ and Morlock, J and Movilla Fernandez and P and Mukherjee, A and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nakano, I and Napier, A and Nett, J and Neu, C and Neubauer, MS and Nielsen, J and Nodulman, L and Noh, SY and Norniella, O and Oakes, L and Oh, SH and Oh,
YD and Oksuzian, I and Okusawa, T and Orava, R and Ortolan, L and Pagan
Griso, S and Pagliarone, C and Palencia, E and Papadimitriou, V and Paramonov, AA and Patrick, J and Pauletta, G and Paulini, M and Paus, C and Pellett, DE and Penzo, A and Phillips, TJ and Piacentino, G and Pianori,
E and Pilot, J and Pitts, K and Plager, C and Pondrom, L and Poprocki, S and Potamianos, K and Prokoshin, F and Pranko, A and Ptohos, F and Punzi, G and Rahaman, A and Ramakrishnan, V and Ranjan, N and Redondo, I and Renton,
P and Rescigno, M and Riddick, T and Rimondi, F and Ristori, L and Robson,
A and Rodrigo, T and Rodriguez, T and Rogers, E and Rolli, S and Roser, R and Ruffini, F and Ruiz, A and Russ, J and Rusu, V and Safonov, A and Sakumoto,
WK and Sakurai, Y and Santi, L and Sato, K and Saveliev, V and Savoy-Navarro, A and Schlabach, P and Schmidt, A and Schmidt, EE and Schwarz, T and Scodellaro, L and Scribano, A and Scuri, F and Seidel, S and Seiya, Y and Semenov, A and Sforza, F and Shalhout, SZ and Shears, T and Shepard, PF and Shimojima, M and Shochet, M and Shreyber-Tecker, I and Simonenko, A and Sinervo, P and Sliwa, K and Smith, JR and Snider, FD and Soha, A and Sorin, V and Song, H and Squillacioti, P and Stancari, M and St
Denis, R and Stelzer, B and Stelzer-Chilton, O and Stentz, D and Strologas, J and Strycker, GL and Sudo, Y and Sukhanov, A and Suslov, I and Takemasa, K and Takeuchi, Y and Tang, J and Tecchio, M and Teng, PK and Thom, J and Thome, J and Thompson, GA and Thomson, E and Toback, D and Tokar, S and Tollefson, K and Tomura, T and Tonelli, D and Torre, S and Torretta, D and Totaro, P and Trovato, M and Ukegawa, F and Uozumi, S and Varganov, A and Vázquez, F and Velev, G and Vellidis, C and Vidal, M and Vila, I and Vilar, R and Vizán, J and Vogel, M and Volpi, G and Wagner, P and Wagner, RL and Wakisaka, T and Wallny, R and Wang, SM and Warburton, A and Waters, D and Wester, WC and Whiteson, D and Wicklund, AB and Wicklund,
E and Wilbur, S and Wick, F and Williams, HH and Wilson, JS and Wilson, P and Winer, BL and Wittich, P and Wolbers, S and Wolfe, H and Wright, T and Wu,
X and Wu, Z and Yamamoto, K and Yamato, D and Yang, T and Yang, UK and Yang,
YC and Yao, W-M and Yeh, GP and Yi, K and Yoh, J and Yorita, K and Yoshida, T and Yu, GB and Yu, I and Yu, SS and Yun, JC and Zanetti, A and Zeng, Y and Zhou,
C and Zucchelli, S and CDF Collaboration},
Title = {Search for the standard model Higgs boson decaying to a bb
pair in events with no charged leptons and large missing
transverse energy using the full CDF data
set.},
Journal = {Physical review letters},
Volume = {109},
Number = {11},
Pages = {111805},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/physrevlett.109.111805},
Abstract = {We report on a search for the standard model Higgs boson
produced in association with a vector boson in the full data
set of proton-antiproton collisions at sqrt[s]=1.96 TeV
recorded by the CDF II detector at the Tevatron,
corresponding to an integrated luminosity of
9.45 fb(-1). We consider events having no identified
charged lepton, a transverse energy imbalance, and two or
three jets, of which at least one is consistent with
originating from the decay of a b quark. We place 95%
credibility level upper limits on the production cross
section times standard model branching fraction for several
mass hypotheses between 90 and 150 GeV/c(2). For a
Higgs boson mass of 125 GeV/c(2), the observed
(expected) limit is 6.7 (3.6) times the standard model
prediction.},
Doi = {10.1103/physrevlett.109.111805},
Key = {fds307686}
}
@article{fds307775,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak,
MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas,
K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Galtieri, AB and Barber,
T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Harpaz,
SB and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen,
K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker,
C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink,
GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic,
I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini,
D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt, O and Bratzler,
U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton, D and Brochu,
FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Renstrom, PABD and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cambiaghi, M and Cameron, D and Caminada,
LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Garrido, MDMC and Caprini,
I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro,
NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung,
SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio,
M and Ciubancan, M and Clark, A and Clark, PJ and Cleland,
W},
Title = {Search for the Standard Model Higgs boson in the decay
channel H→ZZ(*)→4ℓ with 4.8 fb-1
of pp collision data at √s=7 TeV with ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {710},
Number = {3},
Pages = {383-402},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.03.005},
Abstract = {This Letter presents a search for the Standard Model Higgs
boson in the decay channel H→ZZ(*)→ℓ+ℓ-ℓ'+ℓ'-,
where ℓ, ℓ'=e or μ, using proton-proton collisions at
√s=7 TeV recorded with the ATLAS detector and
corresponding to an integrated luminosity of 4.8 fb-1. The
four-lepton invariant mass distribution is compared with
Standard Model background expectations to derive upper
limits on the cross section of a Standard Model Higgs boson
with a mass between 110 GeV and 600 GeV. The mass ranges
134-156 GeV, 182-233 GeV, 256-265 GeV and 268-415 GeV are
excluded at the 95% confidence level. The largest upward
deviations from the background-only hypothesis are observed
for Higgs boson masses of 125 GeV, 244 GeV and 500 GeV with
local significances of 2.1, 2.2 and 2.1 standard deviations,
respectively. Once the look-elsewhere effect is considered,
none of these excesses are significant. © 2012
CERN.},
Doi = {10.1016/j.physletb.2012.03.005},
Key = {fds307775}
}
@article{fds307860,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Search for the Standard Model Higgs boson in the decay
channel H→ZZ(*)→4ℓ with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {705},
Number = {5},
Pages = {435-451},
Publisher = {Elsevier BV},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2011.10.034},
Abstract = {A search for the Standard Model Higgs boson in the decay
channel H→ZZ(*)→ℓ+ℓ-ℓ'+ℓ'-, where ℓ=e, μ, is
presented. Proton-proton collision data at s=7TeV recorded
with the ATLAS detector and corresponding to an average
integrated luminosity of 2.1fb-1 are compared to the
Standard Model expectations. Upper limits on the production
cross section of a Standard Model Higgs boson with a mass
between 110 and 600GeV are derived. The observed (expected)
95% confidence level upper limit on the production cross
section for a Higgs boson with a mass of 194 GeV, the region
with the best expected sensitivity for this search, is 0.99
(1.01) times the Standard Model prediction. The Standard
Model Higgs boson is excluded at 95% confidence level in the
mass ranges 191-197, 199-200 and 214-224 GeV. © 2011
CERN.},
Doi = {10.1016/j.physletb.2011.10.034},
Key = {fds307860}
}
@article{fds307711,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdesselam, A and Abdinov, O and Abi, B and Abolins, M and Abouzeid,
OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Astvatsatourov, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Ay, C and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni,
G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barashkou, A and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall,
A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel, M and Behar
Harpaz, S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Benchouk, C and Bendel, M and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertinelli, F and Bertolucci, F and Besana, MI and Besson, N and Bethke,
S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek,
SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc,
U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Bondarenko, VG and Bondioli, M and Boonekamp, M and Booth,
CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozhko, NI and Bozovic-Jelisavcic, I and Bracinik, J and Braem, A and Branchini, P and Brandenburg, GW and Brandt, A and Brandt, G and Brandt,
O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brelier, B and Bremer, J and Brenner, R and Bressler, S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodbeck, TJ and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, WK and Brown,
G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchanan, NJ and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butin, F and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cambiaghi, M and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo Montoya and GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Cataneo, F and Catinaccio, A and Catmore,
JR and Cattai, A and Cattani, G and Caughron, S and Cauz, D and Cavalleri,
P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Cevenini, F and Chafaq, A and Chakraborty, D and Chan, K and Chapleau,
B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez Barajas and CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, S and Chen, T and Chen, X and Cheng, S and Cheplakov, A and Chepurnov, VF and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciobotaru, MD and Ciocca, C and Ciocio, A and Cirilli, M and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Cleland, W and Clemens, JC},
Title = {Search for the standard model Higgs boson in the diphoton
decay channel with 4.9 fb(-1) of pp collision data at √s=7
TeV with ATLAS.},
Journal = {Physical review letters},
Volume = {108},
Number = {11},
Pages = {111803},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1103/physrevlett.108.111803},
Abstract = {A search for the standard model Higgs boson is performed in
the diphoton decay channel. The data used correspond to an
integrated luminosity of 4.9 fb(-1) collected with the ATLAS
detector at the Large Hadron Collider in proton-proton
collisions at a center-of-mass energy of √s=7 TeV. In the
diphoton mass range 110-150 GeV, the largest excess with
respect to the background-only hypothesis is observed at
126.5 GeV, with a local significance of 2.8 standard
deviations. Taking the look-elsewhere effect into account in
the range 110-150 GeV, this significance becomes 1.5
standard deviations. The standard model Higgs boson is
excluded at 95% confidence level in the mass ranges of
113-115 GeV and 134.5-136 GeV.},
Doi = {10.1103/physrevlett.108.111803},
Key = {fds307711}
}
@article{fds307788,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Arfaoui, S and Arguin J-F., and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov,
A and Artoni, G},
Title = {Search for the Standard Model Higgs boson in the H →
τ+τ- decay mode in √s = 7TeV pp
collisions with ATLAS},
Journal = {Journal of High Energy Physics},
Volume = {2012},
Number = {9},
Publisher = {Springer Nature},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP09(2012)070},
Abstract = {A search for the Standard Model Higgs boson decaying into a
pair of τ leptons is reported. The analysis is based on a
data sample of proton-proton collisions collected by the
ATLAS experiment at the LHC and corresponding to an
integrated luminosity of 4.7fb-1. No significant excess over
the expected background is observed in the Higgs boson mass
range of 100-150 GeV. The observed (expected) upper limits
on the cross section times the branching ratio for H →
τ+τ- are found to be between 2.9 (3.4) and 11.7 (8.2)
times the Standard Model prediction for this mass
range.},
Doi = {10.1007/JHEP09(2012)070},
Key = {fds307788}
}
@article{fds313623,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam,
MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi,
MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga,
XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Costa, JBGD and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Begel,
M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, JB and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botterill, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and Brown, H and Renstrom, PABD and Bruncko,
D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick,
B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Urbán, SC and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan,
P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini, I and Caprini,
M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli,
T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei,
D and Casado, MP and Cascella, M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Gimenez, VC and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda,
V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and Moursli, RCE and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani,
L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, J and Cogneras, E and Colas, J and Colijn, AP and Collins,
NJ and Collins-Tooth, C and Collot, J},
Title = {Search for the Standard Model Higgs boson in the
H→WW({star operator})→ℓνℓν decay mode
with 4.7 fb-1 of ATLAS data at √s=7
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {716},
Number = {1},
Pages = {62-81},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.08.010},
Abstract = {A search for the Standard Model Higgs boson in the
H→WW({star operator})→ℓνℓν (ℓ=e, μ) decay mode
is presented. The search is performed using proton-proton
collision data corresponding to an integrated luminosity of
4.7 fb-1 at a centre-of-mass energy of 7 TeV collected
during 2011 with the ATLAS detector at the Large Hadron
Collider. No significant excess of events over the expected
background is observed. An upper bound is placed on the
Higgs boson production cross section as a function of its
mass. A Standard Model Higgs boson with mass in the range
between 133 GeV and 261 GeV is excluded at 95% confidence
level, while the expected exclusion range is from 127 GeV to
233 GeV. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.08.010},
Key = {fds313623}
}
@article{fds307859,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Search for the Standard Model Higgs boson in the two photon
decay channel with the ATLAS detector at the
LHC},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {705},
Number = {5},
Pages = {452-470},
Publisher = {Elsevier BV},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2011.10.051},
Abstract = {A search for the Standard Model Higgs boson in the two
photon decay channel is reported, using 1.08 fb-1 of
proton-proton collision data at a centre-of-mass energy of 7
TeV recorded by the ATLAS detector. No significant excess is
observed in the investigated mass range of 110-150 GeV.
Upper limits on the cross-section times branching ratio of
between 2.0 and 5.8 times the Standard Model prediction are
derived for this mass range. © 2011 CERN.},
Doi = {10.1016/j.physletb.2011.10.051},
Key = {fds307859}
}
@article{fds321078,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Search for the Standard Model Higgs boson produced by
vector-boson fusion and decaying to bottom quarks in √s=8
TeV pp collisions with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {11},
Publisher = {Springer Nature},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2016)112},
Abstract = {A search with the ATLAS detector is presented for the
Standard Model Higgs boson produced by vector-boson fusion
and decaying to a pair of bottom quarks, using 20.2 fb−1
of LHC proton-proton collision data at s=8 TeV. The signal
is searched for as a resonance in the invariant mass
distribution of a pair of jets containing b-hadrons in
vector-boson-fusion candidate events. The yield is measured
to be −0.8 ± 2.3 times the Standard Model cross-section
for a Higgs boson mass of 125 GeV. The upper limit on the
cross-section times the branching ratio is found to be 4.4
times the Standard Model cross-section at the 95% confidence
level, consistent with the expected limit value of 5.4 (5.7)
in the background-only (Standard Model production)
hypothesis.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP11(2016)112},
Key = {fds321078}
}
@article{fds316850,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for the standard model Higgs boson produced in
association with a vector boson and decaying into a tau pair
in pp collisions at s =8 TeV with the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {93},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {May},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1103/PhysRevD.93.092005},
Abstract = {A search for the standard model Higgs boson produced in
association with a vector boson with the decay H→ττ is
presented. The data correspond to 20.3 fb-1 of integrated
luminosity from proton-proton collisions at s=8 TeV recorded
by the ATLAS experiment at the LHC during 2012. The data
agree with the background expectation, and 95%
confidence-level upper limits are placed on the cross
section of this process. The observed (expected) limit,
expressed in terms of the signal strength μ=σ/σSM for
mH=125 GeV, is μ<5.6 (3.7). The measured value of the
signal strength is μ=2.3±1.6.},
Doi = {10.1103/PhysRevD.93.092005},
Key = {fds316850}
}
@article{fds307657,
Author = {Aad, G and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
TJ and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amonm, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeenm, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Anger, R and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas,
E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal,
V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber,
T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, R and Bartoldus, R and Barton, AE and Bartsch, V and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, R and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall,
AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Bege,
M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell,
PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo,
M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello,
O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge,
D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, R and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bitenc, U and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki,
J and Blonde, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Botteri, D and Bouchami, J and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler,
S and Britton, D and Brochu, FM and Brock, I and Brock, R and Brodet, E and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks,
T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov,
IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock,
AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Campana, S and Campanelli, M and Canale, V and Canelli,
F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido,
MDMC and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casadoll, MP and Cascela,
M and Caso, C and Hernandez, AMC and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Catastini, R and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavalleri, R and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chapleau, B and Chapman, JD and Chapman,
JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen,
Y and Cheplakov, A and El Moursli and RC and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RI and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart,
D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Cogan, JG and Coggeshall, TJ and Cogneras, E and Colas, J and Colijn, AP and Collins,
NJ and Collins-Tooth, C},
Title = {Search for the Standard Model Higgs boson produced in
association with a vector boson and decaying to a
b-quark pair with the ATLAS detector},
Journal = {PHYSICS LETTERS B},
Volume = {718},
Number = {2},
Pages = {369-390},
Publisher = {Elsevier BV},
Year = {2012},
ISSN = {0370-2693},
url = {http://dx.doi.org/10.1016/j.physletb.2012.10.061},
Abstract = {© 2012 CERN This Letter presents the results of a direct
search with the ATLAS detector at the LHC for a Standard
Model Higgs boson of mass 110⩽mH⩽130 GeV produced in
association with a W or Z boson and decaying to bb¯. Three
decay channels are considered: ZH→ℓ+ℓ−bb¯
WH→ℓνbb¯ and ZH→νν¯bb¯ where ℓ corresponds to
an electron or a muon. No evidence for Higgs boson
production is observed in a dataset of 7 TeV pp collisions
corresponding to 4.7 fb−1 of integrated luminosity
collected by ATLAS in 2011. Exclusion limits on Higgs boson
production, at the 95% confidence level, of 2.5 to 5.5 times
the Standard Model cross section are obtained in the mass
range 110–130 GeV. The expected exclusion limits range
between 2.5 and 4.9 for the same mass interval.},
Doi = {10.1016/j.physletb.2012.10.061},
Key = {fds307657}
}
@article{fds307819,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Search for the standard model Higgs boson produced in
association with a W ± boson with 7.5fb
-1 integrated luminosity at CDF},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.86.032011},
Abstract = {We present a search for the standard model Higgs boson
produced in association with a W ± boson. This search uses
data corresponding to an integrated luminosity of 7.5fb -1
collected by the CDF detector at the Tevatron. We select
WH→νbb̄ candidate events with two jets, large missing
transverse energy, and exactly one charged lepton. We
further require that at least one jet be identified to
originate from a bottom quark. Discrimination between the
signal and the large background is achieved through the use
of a Bayesian artificial neural network. The number of
tagged events and their distributions are consistent with
the standard model expectations. We observe no evidence for
a Higgs boson signal and set 95% C.L. upper limits on the WH
production cross section times the branching ratio to decay
to bb̄ pairs, σ(pp̄→W ±H) ×B(H→bb̄), relative to
the rate predicted by the standard model. For the Higgs
boson mass range of 100 to 150GeV/c2 we set observed
(expected) upper limits from 1.34 (1.83) to 38.8 (23.4). For
115GeV/c2 the upper limit is 3.64 (2.78). The combination of
the present search with an independent analysis that selects
events with three jets yields more stringent limits ranging
from 1.12 (1.79) to 34.4 (21.6) in the same mass range. For
115 and 125GeV/c2 the upper limits are 2.65 (2.60) and 4.36
(3.69), respectively. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.86.032011},
Key = {fds307819}
}
@article{fds307821,
Author = {Kotwal, AV and Collaboration, CDF},
Title = {Search for the standard model Higgs boson produced in
association with a Z boson in 7.9/fb of ppbar collisions at
sqrt(s)=1.96 TeV using the CDF II detector},
Journal = {Phys. Lett. B},
Volume = {715},
Number = {1-3},
Pages = {98},
Publisher = {Elsevier BV},
Year = {2012},
Month = {August},
url = {http://dx.doi.org/10.1016/j.physletb.2012.07.045},
Abstract = {We present a search for the standard model Higgs boson
produced in association with a Z boson, using up to 7.9 fb
-1 of integrated luminosity from pp- collisions collected
with the CDF II detector. We utilize several novel
techniques, including multivariate lepton selection,
multivariate trigger parametrization, and a multi-stage
signal discriminant consisting of specialized functions
trained to distinguish individual backgrounds. By increasing
acceptance and enhancing signal discrimination, these
techniques have significantly improved the sensitivity of
the analysis above what was expected from a larger dataset
alone. We observe no significant evidence for a signal, and
we set limits on the ZH production cross section. For a
Higgs boson with mass 115 GeV/c 2, we expect (observe) a
limit of 3.9 (4.8) times the standard model predicted value,
at the 95% credibility level. © 2012 Elsevier
B.V.},
Doi = {10.1016/j.physletb.2012.07.045},
Key = {fds307821}
}
@article{fds356690,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov,
F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini,
MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Antonelli,
M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin,
JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez,
O and Arnold, H and Arratia, M},
Title = {Search for the standard model Higgs boson produced in
association with top quarks and decaying into a bb¯ pair in
pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {97},
Number = {7},
Year = {2018},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.97.072016},
Abstract = {A search for the standard model Higgs boson produced in
association with a top-quark pair, ttH, is presented. The
analysis uses 36.1 fb-1 of pp collision data at s=13 TeV
collected with the ATLAS detector at the Large Hadron
Collider in 2015 and 2016. The search targets the H→bb
decay mode. The selected events contain either one or two
electrons or muons from the top-quark decays, and are then
categorized according to the number of jets and how likely
these are to contain b-hadrons. Multivariate techniques are
used to discriminate between signal and background events,
the latter being dominated by tt+jets production. For a
Higgs boson mass of 125 GeV, the ratio of the measured ttH
signal cross-section to the standard model expectation is
found to be μ=0.84-0.61+0.64. A value of μ greater than
2.0 is excluded at 95% confidence level (C.L.) while the
expected upper limit is μ<1.2 in the absence of a ttH
signal.},
Doi = {10.1103/PhysRevD.97.072016},
Key = {fds356690}
}
@article{fds310331,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Piqueras, DÁ and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagiacchi, P and Bagnaia,
P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis,
D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro
Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen,
S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard,
NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Buszello, CP and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, R and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana,
S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton, DG and Chau, CC and Chavez
Barajas, CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella,
V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly, IA and Consonni, SM and Consorti, V and Constantinescu, S and Conta,
C},
Title = {Search for the Standard Model Higgs boson produced in
association with top quarks and decaying into [Formula: see
text] in [Formula: see text] collisions at [Formula: see
text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {7},
Pages = {349},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3543-1},
Abstract = {A search for the Standard Model Higgs boson produced in
association with a top-quark pair, [Formula: see text], is
presented. The analysis uses 20.3 fb<sup>-1</sup> of
<i>pp</i> collision data at [Formula: see text], collected
with the ATLAS detector at the Large Hadron Collider during
2012. The search is designed for the [Formula: see text]
decay mode and uses events containing one or two electrons
or muons. In order to improve the sensitivity of the search,
events are categorised according to their jet and
<i>b</i>-tagged jet multiplicities. A neural network is used
to discriminate between signal and background events, the
latter being dominated by [Formula: see text]+jets
production. In the single-lepton channel, variables
calculated using a matrix element method are included as
inputs to the neural network to improve discrimination of
the irreducible [Formula: see text] background. No
significant excess of events above the background
expectation is found and an observed (expected) limit of 3.4
(2.2) times the Standard Model cross section is obtained at
95 % confidence level. The ratio of the measured [Formula:
see text] signal cross section to the Standard Model
expectation is found to be [Formula: see text] assuming a
Higgs boson mass of 125[Formula: see text].},
Doi = {10.1140/epjc/s10052-015-3543-1},
Key = {fds310331}
}
@article{fds310311,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for the Xb and other hidden-beauty states
in the π+π−ϒ(1S) channel at
ATLAS},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {740},
Pages = {199-217},
Publisher = {Elsevier BV},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2014.11.055},
Abstract = {This Letter presents a search for a hidden-beauty
counterpart of the X(3872) in the mass ranges of
10.05–10.31 GeV and 10.40–11.00 GeV, in the channel
Xb→π+π−ϒ(1S)(→μ+μ−), using 16.2 fb−1 of s=8
TeV pp collision data collected by the ATLAS detector at the
LHC. No evidence for new narrow states is found, and upper
limits are set on the product of the Xb cross section and
branching fraction, relative to those of the ϒ(2S), at the
95% confidence level using the CLS approach. These limits
range from 0.8% to 4.0%, depending on mass. For masses above
10.1 GeV, the expected upper limits from this analysis are
the most restrictive to date. Searches for production of the
ϒ(13DJ), ϒ(10860), and ϒ(11020) states also reveal no
significant signals.},
Doi = {10.1016/j.physletb.2014.11.055},
Key = {fds310311}
}
@article{fds376063,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye,
T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal,
A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja,
S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh,
B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Alviggi, MG and Aly, M and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L},
Title = {Search for the Zγ decay mode of new high-mass resonances in
pp collisions at s=13 TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {848},
Year = {2024},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2023.138394},
Abstract = {This letter presents a search for narrow, high-mass
resonances in the Zγ final state with the Z boson decaying
into a pair of electrons or muons. The s=13 TeV pp collision
data were recorded by the ATLAS detector at the CERN Large
Hadron Collider and have an integrated luminosity of 140
fb−1. The data are found to be in agreement with the
Standard Model background expectation. Upper limits are set
on the resonance production cross section times the decay
branching ratio into Zγ. For spin-0 resonances produced via
gluon–gluon fusion, the observed limits at 95% confidence
level vary between 65.5 fb and 0.6 fb, while for spin-2
resonances produced via gluon–gluon fusion (or
quark–antiquark initial states) limits vary between 77.4
(76.1) fb and 0.6 (0.5) fb, for the mass range from 220 GeV
to 3400 GeV.},
Doi = {10.1016/j.physletb.2023.138394},
Key = {fds376063}
}
@article{fds307887,
Author = {Aaltonen, TEA},
Title = {Search for the {H}iggs boson in the all-hadronic final state
using the {CDF II} detector},
Journal = {Phys. Rev. D},
Volume = {84},
Number = {5},
Pages = {052010},
Publisher = {American Physical Society},
Year = {2011},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.84.052010},
Abstract = {We report on a search for the production of the Higgs boson
decaying to two bottom quarks accompanied by two additional
quarks. The data sample used corresponds to an integrated
luminosity of approximately 4fb-1 of pp̄ collisions at
√s=1.96TeV recorded by the CDF II experiment. This search
includes twice the integrated luminosity of the previous
published result, uses analysis techniques to distinguish
jets originating from light flavor quarks and those from
gluon radiation, and adds sensitivity to a Higgs boson
produced by vector boson fusion. We find no evidence of the
Higgs boson and place limits on the Higgs boson production
cross section for Higgs boson masses between 100GeV/c2 and
150GeV/c2 at the 95% confidence level. For a Higgs boson
mass of 120GeV/c2, the observed (expected) limit is 10.5
(20.0) times the predicted standard model cross section. ©
2011 American Physical Society.},
Doi = {10.1103/PhysRevD.84.052010},
Key = {fds307887}
}
@article{fds307651,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov,
VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Search for third generation scalar leptoquarks in pp
collisions at √s=7 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2013},
Number = {6},
Publisher = {Springer Nature},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP06(2013)033},
Abstract = {A search for pair-produced third generation scalar
leptoquarks is presented, using proton-proton collisions at
s=7 TeV at the LHC. The data were recorded with the ATLAS
detector and correspond to an integrated luminosity of 4.7
fb-1. Each leptoquark is assumed to decay to a tau lepton
and a b-quark with a branching fraction equal to 100%. No
statistically significant excess above the Standard Model
expectation is observed. Third generation leptoquarks are
therefore excluded at 95% confidence level for masses less
than 534GeV. [Figure not available: see fulltext.] © 2013
Cern for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP06(2013)033},
Key = {fds307651}
}
@article{fds307684,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for top and bottom squarks from gluino pair
production in final states with missing transverse energy
and at least three b-jets with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {72},
Number = {10},
Publisher = {Springer Nature},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1140/epjc/s10052-012-2174-z},
Abstract = {This letter reports the results of a search for top and
bottom squarks from gluino pair production in 4.7 fb−1of
pp collisions at √s = 7 TeV using the ATLAS detector at
the LHC. The search is performed in events with large
missing transverse momentum and at least three jets
identified as originating from a b-quark. Exclusion limits
are presented for a variety of gluino-mediated models with
gluino masses up to 1 TeV excluded.},
Doi = {10.1140/epjc/s10052-012-2174-z},
Key = {fds307684}
}
@article{fds313585,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison,
LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson,
KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Arnaez, O},
Title = {Search for top quark decays t → qH with H → γγ using
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {6},
Year = {2014},
Month = {January},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP06(2014)008},
Abstract = {A search is performed for flavour-changing neutral currents
in the decay of a top quark to an up-type (c, u) quark and a
Higgs boson, where the Higgs boson decays to two photons.
The proton-proton collision data set used corresponds to 4.7
fb-1 at √ = 7TeV and 20.3fb-1 at √ = 8TeV collected by
the ATLAS experiment at the LHC. Top quark pair events are
searched for in which one top quark decays to qH and the
other decays to bW. Both the hadronic and the leptonic decay
modes of the W boson are used. No significant signal is
observed and an upper limit is set on the t → qH branching
ratio of 0.79 at the 95% confidence level. The corresponding
limit on the tqH coupling combination λtcH2 + λtuH2 is
0.17. © 2014 The Author(s).},
Doi = {10.1007/JHEP06(2014)008},
Key = {fds313585}
}
@article{fds356732,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ},
Title = {Search for top quark decays t → qH, with H → γγ, in
√s=13 TeV pp collisions using the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {10},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2017)129},
Abstract = {This article presents a search for flavour-changing neutral
currents in the decay of a top quark into an up-type (q = c,
u) quark and a Higgs boson, where the Higgs boson decays
into two photons. The proton-proton collision data set
analysed amounts to 36.1 fb−1 at s=13 TeV collected by the
ATLAS experiment at the LHC. Top quark pair events are
searched for, where one top quark decays into qH and the
other decays into bW. Both the hadronic and leptonic decay
modes of the W boson are used. No significant excess is
observed and an upper limit is set on the t → cH branching
ratio of 2.2 × 10−3 at the 95% confidence level, while
the expected limit in the absence of signal is 1.6 ×
10−3. The corresponding limit on the tcH coupling is 0.090
at the 95% confidence level. The observed upper limit on the
t → uH branching ratio is 2.4 × 10−3.[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP10(2017)129},
Key = {fds356732}
}
@article{fds310348,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez,
O},
Title = {Search for top squark pair production in final states with
one isolated lepton, jets, and missing transverse momentum
in √ s = 8 TeV pp collisions with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2014},
Number = {11},
Publisher = {Springer Nature},
Year = {2014},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2014)118},
Abstract = {The results of a search for top squark (stop) pair
production in final states with one isolated lepton, jets,
and missing transverse momentum are reported. The analysis
is performed with proton-proton collision data at (Formula
presented.) = 8 TeV collected with the ATLAS detector at the
LHC in 2012 corresponding to an integrated luminosity of 20
fb−1. The lightest supersymmetric particle (LSP) is taken
to be the lightest neutralino which only interacts weakly
and is assumed to be stable. The stop decay modes considered
are those to a top quark and the LSP as well as to a bottom
quark and the lightest chargino, where the chargino decays
to the LSP by emitting a W boson. A wide range of scenarios
with different mass splittings between the stop, the
lightest neutralino and the lightest chargino are
considered, including cases where the W bosons or the top
quarks are off-shell. Decay modes involving the heavier
charginos and neutralinos are addressed using a set of
phenomenological models of supersymmetry. No significant
excess over the Standard Model prediction is observed. A
stop with a mass between 210 and 640 GeV decaying directly
to a top quark and a massless LSP is excluded at 95%
confidence level, and in models where the mass of the
lightest chargino is twice that of the LSP, stops are
excluded at 95% confidence level up to a mass of 500 GeV for
an LSP mass in the range of 100 to 150 GeV. Stringent
exclusion limits are also derived for all other stop decay
modes considered, and model-independent upper limits are set
on the visible cross-section for processes beyond the
Standard Model.},
Doi = {10.1007/JHEP11(2014)118},
Key = {fds310348}
}
@booklet{Abachi98,
Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Álvarez, G and Alves,
GA and Amidi, E and Amos, N and Anderson, EW and Aronson, SH and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Bendich, J and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Bischoff, A and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt,
A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty,
D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and De,
K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard,
J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahey, S and Fahland, T and Fatyga, M and Fatyga, MK and Featherly, J and Feher, S},
Title = {Search for top squark pair production in the dielectron
channel},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {57},
Number = {1},
Pages = {589-593},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.57.589},
Abstract = {This report describes the first search for top squark pair
production in the channel (Formula presented)+jets+(Formula
presented) using (Formula presented) pb(Formula presented)
of data collected using the DØ detector. A 95% confidence
level upper limit on (Formula presented) is presented. The
limit is above the theoretical expectation for (Formula
presented) for this process, but does show the sensitivity
of the current DØ data set to a particular topology for new
physics. © 1998 The American Physical Society.},
Doi = {10.1103/PhysRevD.57.589},
Key = {Abachi98}
}
@article{fds356673,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke,
BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amoroso, S and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antonov, A and Antrim, DJA and Anulli, F and Aoki,
M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Arnaez, O and Arnold, H and Arratia, M},
Title = {Search for top squarks decaying to tau sleptons in pp
collisions at s =13 Te v with the ATLAS detector},
Journal = {Physical Review D},
Volume = {98},
Number = {3},
Year = {2018},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.98.032008},
Abstract = {A search for direct pair production of top squarks in final
states with two tau leptons, b-jets, and missing transverse
momentum is presented. The analysis is based on
proton-proton collision data at s=13 TeV corresponding to an
integrated luminosity of 36.1 fb-1 recorded with the ATLAS
detector at the Large Hadron Collider in 2015 and 2016. Two
exclusive channels with either two hadronically decaying tau
leptons or one hadronically and one leptonically decaying
tau lepton are considered. No significant deviation from the
Standard Model predictions is observed in the data. The
analysis results are interpreted in terms of
model-independent limits and used to derive exclusion limits
on the masses of the top squark t1 and the tau slepton τ1
in a simplified model of supersymmetry with a nearly
massless gravitino. In this model, masses up to m(t1)=1.16
TeV and m(τ1)=1.00 TeV are excluded at 95% confidence
level.},
Doi = {10.1103/PhysRevD.98.032008},
Key = {fds356673}
}
@article{fds353613,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Barrio, NA and Ferraz, VA and Pereira, RA},
Title = {Search for top squarks in events with a Higgs or Z boson
using 139 fb - 1 of pp collision data at √s=13
TeV with the ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {11},
Year = {2020},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-08469-8},
Abstract = {This paper presents a search for direct top squark pair
production in events with missing transverse momentum plus
either a pair of jets consistent with Standard Model Higgs
boson decay into b-quarks or a same-flavour opposite-sign
dilepton pair with an invariant mass consistent with a Z
boson. The analysis is performed using the proton–proton
collision data at s=13 TeV collected with the ATLAS detector
during the LHC Run-2, corresponding to an integrated
luminosity of 139 fb- 1. No excess is observed in the data
above the Standard Model predictions. The results are
interpreted in simplified models featuring direct production
of pairs of either the lighter top squark (t~ 1) or the
heavier top squark (t~ 2), excluding at 95% confidence level
t~ 1 and t~ 2 masses up to about 1220 and 875 GeV,
respectively.},
Doi = {10.1140/epjc/s10052-020-08469-8},
Key = {fds353613}
}
@article{fds321099,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abouzeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H},
Title = {Search for top squarks in final states with one isolated
lepton, jets, and missing transverse momentum in s =13 TeV
pp collisions with the ATLAS detector},
Journal = {Physical Review D},
Volume = {94},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.94.052009},
Abstract = {The results of a search for the top squark, the
supersymmetric partner of the top quark, in final states
with one isolated electron or muon, jets, and missing
transverse momentum are reported. The search uses the 2015
LHC pp collision data at a center-of-mass energy of s=13 TeV
recorded by the ATLAS detector and corresponding to an
integrated luminosity of 3.2 fb-1. The analysis targets two
types of signal models: gluino-mediated pair production of
top squarks with a nearly mass-degenerate top squark and
neutralino and direct pair production of top squarks,
decaying to the top quark and the lightest neutralino. The
experimental signature in both signal scenarios is similar
to that of a top quark pair produced in association with
large missing transverse momentum. No significant excess
over the Standard Model background prediction is observed,
and exclusion limits on gluino and top squark masses are set
at 95% confidence level. The results extend the LHC run-1
exclusion limit on the gluino mass up to 1460 GeV in the
gluino-mediated scenario in the high gluino and low top
squark mass region and add an excluded top squark mass
region from 745 to 780 GeV for the direct top squark model
with a massless lightest neutralino. The results are also
reinterpreted to set exclusion limits in a model of
vectorlike top quarks.},
Doi = {10.1103/PhysRevD.94.052009},
Key = {fds321099}
}
@article{fds356597,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA},
Title = {Search for top-quark decays t → Hq with 36
fb−1 of pp collision data at √s = 13 TeV with
the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1007/JHEP05(2019)123},
Abstract = {A search for flavour-changing neutral current decays of a
top quark into an up-type quark (q = u, c) and the Standard
Model Higgs boson, t → Hq, is presented. The search is
based on a dataset of pp collisions at s = 13 TeV recorded
in 2015 and 2016 with the ATLAS detector at the CERN Large
Hadron Collider and corresponding to an integrated
luminosity of 36.1 fb−1. Two complementary analyses are
performed to search for top-quark pair events in which one
top quark decays into Wb and the other top quark decays into
Hq, and target the H→ bb¯ and H → τ+τ− decay modes,
respectively. The high multiplicity of b-quark jets, or the
presence of hadronically decaying τ-leptons, is exploited
in the two analyses respectively. Multivariate techniques
are used to separate the signal from the background, which
is dominated by top-quark pair production. No significant
excess of events above the background expectation is found,
and 95% CL upper limits on the t → Hq branching ratios are
derived. The combination of these searches with ATLAS
searches in diphoton and multilepton final states yields
observed (expected) 95% CL upper limits on the t → Hc and
t → Hu branching ratios of 1.1 × 10−3 (8.3 × 10−4)
and 1.2 × 10−3 (8.3 × 10−4), respectively. The
corresponding combined observed (expected) upper limits on
the |λtcH| and |λtuH| couplings are 0.064 (0.055) and
0.066 (0.055), respectively.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP05(2019)123},
Key = {fds356597}
}
@article{fds307955,
Author = {Aaltonen, T and others},
Title = {Search for Top-Quark Production via Flavor-Changing Neutral
Currents in W + 1 Jet Events at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {102},
Number = {15},
Pages = {151801},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/physrevlett.102.151801},
Abstract = {We report on a search for the non-standard-model process
u(c) + g --> t using pp[over ] collision data collected by
the Collider Detector at Fermilab II detector corresponding
to 2.2 fb;{-1}. The candidate events are classified as
signal-like or backgroundlike by an artificial neural
network. The observed discriminant distribution yields no
evidence for flavor-changing neutral current top-quark
production, resulting in an upper limit on the production
cross section sigma(u(c) + g --> t) < 1.8 pb at the 95% C.L.
Using theoretical predictions we convert the cross section
limit to upper limits on flavor-changing neutral current
branching ratios: B(t --> u + g) < 3.9 x 10;{-4} and B(t -->
c + g) < 5.7 x 10;{-3}.},
Doi = {10.1103/physrevlett.102.151801},
Key = {fds307955}
}
@article{fds336452,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for top-squark pair production in final states with
one lepton, jets, and missing transverse momentum using 36
fb−1 of √s=13 TeV pp collision data with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {6},
Publisher = {Springer Nature},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2018)108},
Abstract = {The results of a search for the direct pair production of
top squarks, the supersymmetric partner of the top quark, in
final states with one isolated electron or muon, several
energetic jets, and missing transverse momentum are
reported. The analysis also targets spin-0 mediator models,
where the mediator decays into a pair of dark-matter
particles and is produced in association with a pair of top
quarks. The search uses data from proton-proton collisions
delivered by the Large Hadron Collider in 2015 and 2016 at a
centre-of-mass energy of s=13 TeV and recorded by the ATLAS
detector, corresponding to an integrated luminosity of 36
fb−1. A wide range of signal scenarios with different
mass-splittings between the top squark, the lightest
neutralino and possible intermediate supersymmetric
particles are considered, including cases where the W bosons
or the top quarks produced in the decay chain are off-shell.
No significant excess over the Standard Model prediction is
observed. The null results are used to set exclusion limits
at 95% confidence level in several supersymmetry benchmark
models. For pair-produced top-squarks decaying into top
quarks, top-squark masses up to 940 GeV are excluded.
Stringent exclusion limits are also derived for all other
considered top-squark decay scenarios. For the spin-0
mediator models, upper limits are set on the visible
cross-section.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP06(2018)108},
Key = {fds336452}
}
@article{fds347494,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and Bilbao
De Mendizabal and J and Billoud, TRV and Bilokon, H and Bindi, M and Binet,
S and Bingul, A and Bini, C and Biondi, S and Bisanz, T and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge,
MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister,
I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey,
P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Callea, G and Caloba,
LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal
Armadans, R and Camincher, C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Cano Bret,
M and Cantero, J and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo,
F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Castillo
Gimenez, V and Castro, NF and Catinaccio, A and Catmore, JR and Cattai,
A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerda
Alberich, L and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev,
SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan,
M},
Title = {Search for triboson [Formula: see text] production in
pp collisions at [Formula: see text] [Formula: see
text] with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {3},
Pages = {141},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-4692-1},
Abstract = {This paper reports a search for triboson [Formula: see text]
production in two decay channels ([Formula: see text] and
[Formula: see text] with [Formula: see text]) in
proton-proton collision data corresponding to an integrated
luminosity of 20.3 [Formula: see text] at a centre-of-mass
energy of 8 [Formula: see text] with the ATLAS detector at
the Large Hadron Collider. Events with exactly three charged
leptons, or two leptons with the same electric charge in
association with two jets, are selected. The total number of
events observed in data is consistent with the Standard
Model (SM) predictions. The observed 95% confidence level
upper limit on the SM [Formula: see text] production cross
section is found to be 730 fb with an expected limit of 560
fb in the absence of SM [Formula: see text] production.
Limits are also set on <i>WWWW</i> anomalous quartic gauge
couplings.},
Doi = {10.1140/epjc/s10052-017-4692-1},
Key = {fds347494}
}
@booklet{Abbott98n,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson,
EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis,
E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram,
I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho,
W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto,
G and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E and Forden, GE},
Title = {Search for trilepton signatures from associated gaugino pair
production},
Journal = {Physical Review Letters},
Volume = {80},
Number = {8},
Pages = {1591-1596},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevLett.80.1591},
Abstract = {We report on a search for the trilepton decay signature from
the associated production of supersymmetric gaugino pairs,
χ∼±1χ∼02, within the context of minimal
supersymmetric models that conserve R parity. This search
uses 95 pb−1 of pp− data taken at s = 1.8 TeV with the
D0 detector. No evidence of a trilepton signature has been
found, and a limit on the product of cross section times
branching fraction to trileptons is given as a function of
χ∼±1 mass. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.80.1591},
Key = {Abbott98n}
}
@article{fds221244,
Author = {A.V. Kotwal and G. Aad et al (ATLAS Collaboration)},
Title = {Search for ttbar resonances in the lepton plus jets final
state with ATLAS using 4.7 / fb of pp collisions at
sqrt(s)=7 TeV},
Journal = {Phys. Rev. D},
Volume = {88},
Number = {012004},
Year = {2013},
Month = {July},
Key = {fds221244}
}
@article{fds352786,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Aranzabal
Barrio, N and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C},
Title = {Search for tt¯ resonances in fully hadronic final states in
pp collisions at √s = 13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2020},
Number = {10},
Year = {2020},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2020)061},
Abstract = {This paper presents a search for new heavy particles
decaying into a pair of top quarks using 139 fb−1 of
proton-proton collision data recorded at a centre-of-mass
energy of s = 13 TeV with the ATLAS detector at the Large
Hadron Collider. The search is performed using events
consistent with pair production of high-transverse-momentum
top quarks and their subsequent decays into the fully
hadronic final states. The analysis is optimized for
resonances decaying into a tt¯ pair with mass above 1.4
TeV, exploiting a dedicated multivariate technique with jet
substructure to identify hadronically decaying top quarks
using large-radius jets and evaluating the background
expectation from data. No significant deviation from the
background prediction is observed. Limits are set on the
production cross-section times branching fraction for the
new Z′ boson in a topcolor-assisted-technicolor model. The
Z′ boson masses below 3.9 and 4.7 TeV are excluded at 95%
confidence level for the decay widths of 1% and 3%,
respectively. [Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2020)061},
Key = {fds352786}
}
@article{fds307590,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Search for tt̄ resonances in the lepton plus jets final
state with ATLAS using 4.7 fb–1of pp collisions
at √s = 7 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.88.012004},
Abstract = {A search for new particles that decay into top quark pairs
(tt) is performed with the ATLAS experiment at the LHC using
an integrated luminosity of 4.7 fb–1of proton–proton
(pp) collision data collected at a center-of-mass energy
√s = 7 TeV. In the tt̄→ WbWb decay, the lepton plus
jets final state is used, where one W boson decays
leptonically and the other hadronically. The tt̄system is
reconstructed using both small-radius and large-radius jets,
the latter being supplemented by a jet substructure
analysis. A search for local excesses in the number of data
events compared to the Standard Model expectation in the
tt̄invariant mass spectrum is performed. No evidence for a
tt̄resonance is found and 95% credibility-level limits on
the production rate are determined for massive states
predicted in two benchmark models. The upper limits on the
cross section times branching ratio of a narrow Z′
resonance range from 5.1 pb for a boson mass of 0.5 TeV to
0.03 pb for a mass of 3 TeV. A narrow leptophobic topcolor
Z′ resonance with a mass below 1.74 TeV is excluded.
Limits are also derived for a broad color-octet resonance
with Γ/m = 15.3%. A Kaluza–Klein excitation of the gluon
in a Randall–Sundrum model is excluded for masses below
2.07 TeV.},
Doi = {10.1103/PhysRevD.88.012004},
Key = {fds307590}
}
@article{fds355554,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury,
KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Search for type-III seesaw heavy leptons in dilepton final
states in pp collisions at √s=13TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {81},
Number = {3},
Year = {2021},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-08929-9},
Abstract = {A search for the pair production of heavy leptons as
predicted by the type-III seesaw mechanism is presented. The
search uses proton–proton collision data at a
centre-of-mass energy of 13 TeV, corresponding to 139fb-1
of integrated luminosity recorded by the ATLAS detector
during Run 2 of the Large Hadron Collider. The analysis
focuses on the final state with two light leptons (electrons
or muons) of different flavour and charge combinations, with
at least two jets and large missing transverse momentum. No
significant excess over the Standard Model expectation is
observed. The results are translated into exclusion limits
on heavy-lepton masses, and the observed lower limit on the
mass of the type-III seesaw heavy leptons is 790 GeV at 95%
confidence level.},
Doi = {10.1140/epjc/s10052-021-08929-9},
Key = {fds355554}
}
@article{fds367719,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al
Khoury, K and Alberghi, GL and Albert, J and Albicocco, P and Alconada
Verzini, MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin,
JF},
Title = {Search for type-III seesaw heavy leptons in leptonic final
states in pp collisions at √s=13TeV with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {82},
Number = {11},
Year = {2022},
Month = {November},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10785-0},
Abstract = {A search for the pair production of heavy leptons as
predicted by the type-III seesaw mechanism is presented. The
search uses proton–proton collision data at a
centre-of-mass energy of 13 TeV, corresponding to 139fb-1
of integrated luminosity recorded by the ATLAS detector
during Run 2 of the Large Hadron Collider. The analysis
focuses on final states with three or four electrons or
muons from the possible decays of new heavy leptons via
intermediate electroweak bosons. No significant deviations
above the Standard Model expectation are observed; upper and
lower limits on the heavy lepton production cross-section
and masses are derived respectively. These results are then
combined for the first time with the ones already published
by ATLAS using the channel with two leptons in the final
state. The observed lower limit on the mass of the type-III
seesaw heavy leptons combining two, three and four lepton
channels together is 910 GeV at the 95% confidence
level.},
Doi = {10.1140/epjc/s10052-022-10785-0},
Key = {fds367719}
}
@article{fds310267,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Search for type-III seesaw heavy leptons in pp collisions at
s =8 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.92.032001},
Abstract = {A search for the pair production of heavy leptons (N0,L±)
predicted by the type-III seesaw theory formulated to
explain the origin of small neutrino masses is presented.
The decay channels N0→W±l (=e,μ,τ) and L±→W±ν
(ν=νe,νμ,ντ) are considered. The analysis is performed
using the final state that contains two leptons (electrons
or muons), two jets from a hadronically decaying W boson and
large missing transverse momentum. The data used in the
measurement correspond to an integrated luminosity of 20.3
fb-1 of pp collisions at s=8 TeV collected by the ATLAS
detector at the LHC. No evidence of heavy lepton pair
production is observed. Heavy leptons with masses below
325-540 GeV are excluded at the 95% confidence level,
depending on the theoretical scenario considered.},
Doi = {10.1103/PhysRevD.92.032001},
Key = {fds310267}
}
@article{fds308062,
Author = {Abulencia, and A, and others},
Title = {Search for V + A current in top quark decay in p anti-p
collisions at s**(1/2) = 1.96-TeV},
Journal = {Phys. Rev. Lett.},
Volume = {98},
Number = {7},
Pages = {072001},
Year = {2007},
url = {http://dx.doi.org/10.1103/physrevlett.98.072001},
Abstract = {We report an upper limit on the fraction of V+A current,
fV+A, in top-quark decays, using approximately 700 pb-1 of
p[overline p] collisions at sqrt(s)=1.96 TeV acquired by the
upgraded Collider Detector at Fermilab. For the decay
t-->Wb-->[script-l]nub (where [script-l]=e or µ), the
invariant mass of the charged lepton and the bottom quark
jet is sensitive to the polarization of the W boson. We
determine fV+A=-0.06$\pm$0.25 given a top-quark mass of 175
GeV/c2. We set an upper limit on fV+A of 0.29 at the 95\%
confidence level, an improvement by a factor of 2 on the
previous best direct limit.},
Doi = {10.1103/physrevlett.98.072001},
Key = {fds308062}
}
@article{fds356630,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel,
C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP and Araujo Ferraz and V and Araujo Pereira and R and Arce, ATH and Ardell,
RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ},
Title = {Search for vector-boson resonances decaying to a top quark
and bottom quark in the lepton plus jets final state in pp
collisions at √s=13TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {788},
Pages = {347-370},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2018.11.032},
Abstract = {A search for new charged massive gauge bosons, W′, is
performed with the ATLAS detector at the LHC. Data were
collected in proton–proton collisions at a center-of-mass
energy of s=13 TeV and correspond to an integrated
luminosity of 36.1 fb−1. This analysis searches for W′
bosons in the W′→tb¯ decay channel in final states with
an electron or muon plus jets. The search covers resonance
masses between 0.5 and 5.0 TeV and considers right-handed
W′ bosons. No significant deviation from the Standard
Model (SM) expectation is observed and upper limits are set
on the W′→tb¯ cross section times branching ratio and
the W′ boson effective couplings as a function of the W′
boson mass. For right-handed W′ bosons with coupling to
the SM particles equal to the SM weak coupling constant,
masses below 3.15 TeV are excluded at the 95% confidence
level. This search is also combined with a previously
published ATLAS result for W′→tb¯ in the fully hadronic
final state. Using the combined searches, right-handed W′
bosons with masses below 3.25 TeV are excluded at the 95%
confidence level.},
Doi = {10.1016/j.physletb.2018.11.032},
Key = {fds356630}
}
@article{fds310281,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov,
AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G},
Title = {Search for vectorlike B quarks in events with one isolated
lepton, missing transverse momentum, and jets at s =8 TeV
with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {11},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.91.112011},
Abstract = {A search has been performed for pair production of heavy
vectorlike down-type (B) quarks. The analysis explores the
lepton-plus-jets final state, characterized by events with
one isolated charged lepton (electron or muon), significant
missing transverse momentum, and multiple jets. One or more
jets are required to be tagged as arising from b quarks, and
at least one pair of jets must be tagged as arising from the
hadronic decay of an electroweak boson. The analysis uses
the full data sample of pp collisions recorded in 2012 by
the ATLAS detector at the LHC, operating at a center-of-mass
energy of 8 TeV, corresponding to an integrated luminosity
of 20.3 fb-1. No significant excess of events is observed
above the expected background. Limits are set on vectorlike
B production, as a function of the B branching ratios,
assuming the allowable decay modes are B→Wt/Zb/Hb. In the
chiral limit with a branching ratio of 100% for the decay
B→Wt, the observed (expected) 95% C.L. lower limit on the
vectorlike B mass is 810 GeV (760 GeV). In the case where
the vectorlike B quark has branching ratio values
corresponding to those of an SU(2) singlet state, the
observed (expected) 95% C.L. lower limit on the vectorlike B
mass is 640 GeV (505 GeV). The same analysis, when used to
investigate pair production of a colored, charge 5/3 exotic
fermion T5/3, with subsequent decay T5/3→Wt, sets an
observed (expected) 95% C.L. lower limit on the T5/3 mass of
840 GeV (780 GeV).},
Doi = {10.1103/PhysRevD.91.112011},
Key = {fds310281}
}
@article{fds356691,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Search for W W/W Z resonance production in ℓνqq final
states in pp collisions at √s=13 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {3},
Year = {2018},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2018)042},
Abstract = {A search is conducted for new resonances decaying into a W W
or W Z boson pair, where one W boson decays leptonically and
the other W or Z boson decays hadronically. It is based on
proton-proton collision data with an integrated luminosity
of 36.1 fb−1 collected with the ATLAS detector at the
Large Hadron Collider at a centre-of-mass energy of s=13 TeV
in 2015 and 2016. The search is sensitive to diboson
resonance production via vector-boson fusion as well as
quark-antiquark annihilation and gluon-gluon fusion
mechanisms. No significant excess of events is observed with
respect to the Standard Model backgrounds. Several benchmark
models are used to interpret the results. Limits on the
production cross section are set for a new narrow scalar
resonance, a new heavy vector-boson and a spin-2
Kaluza-Klein graviton.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP03(2018)042},
Key = {fds356691}
}
@article{fds310313,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V},
Title = {Search for W ′ → t b ¯ in the lepton plus jets final
state in proton–proton collisions at a centre-of-mass
energy of s = 8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {743},
Pages = {235-255},
Publisher = {Elsevier BV},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1016/j.physletb.2015.02.051},
Abstract = {A search for new charged massive gauge bosons, called W′,
is performed with the ATLAS detector at the LHC, in
proton–proton collisions at a centre-of-mass energy of s=8
TeV, using a dataset corresponding to an integrated
luminosity of 20.3 fb−1. This analysis searches for W′
bosons in the W′→tb¯ decay channel in final states with
electrons or muons, using a multivariate method based on
boosted decision trees. The search covers masses between 0.5
and 3.0 TeV, for right-handed or left-handed W′ bosons. No
significant deviation from the Standard Model expectation is
observed and limits are set on the W′→tb¯ cross-section
times branching ratio and on the W′-boson effective
couplings as a function of the W′-boson mass using the CLs
procedure. For a left-handed (right-handed) W′ boson,
masses below 1.70 (1.92) TeV are excluded at 95% confidence
level.},
Doi = {10.1016/j.physletb.2015.02.051},
Key = {fds310313}
}
@article{fds308078,
Author = {Abulencia, and A, and others},
Title = {Search for W' boson decaying to electron-neutrino pairs in p
anti-p collisions at s**(1/2) = 1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D75},
Number = {9},
Pages = {091101},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.75.091101},
Abstract = {We present the results of a search for W[prime] boson
decaying to electron-neutrino pairs in p[overline p]
collisions at a center-of-mass energy of 1.96 TeV, using a
data sample corresponding to 205 pb-1 of integrated
luminosity collected by the CDF II detector at Fermilab. We
observe no evidence for this decay mode and set limits on
the production cross section times branching fraction,
assuming the neutrinos from W[prime] boson decays to be
light. If we assume the manifest left-right symmetric model,
we exclude a W[prime] boson with mass less than 788 GeV/c2
at the 95\% confidence level.},
Doi = {10.1103/PhysRevD.75.091101},
Key = {fds308078}
}
@article{fds307605,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik, E and Arik, M},
Title = {Search for WH production with a light Higgs boson decaying
to prompt electron-jets in proton-proton collisions at
√s=7 TeV with the ATLAS detector},
Journal = {New Journal of Physics},
Volume = {15},
Number = {4},
Pages = {043009-043009},
Publisher = {IOP Publishing},
Year = {2013},
Month = {April},
url = {http://dx.doi.org/10.1088/1367-2630/15/4/043009},
Abstract = {A search is performed for WH production with a light Higgs
boson decaying to hidden-sector particles resulting in
clusters of collimated electrons, known as electron-jets.
The search is performed with 2.04 fb-1 of data collected in
2011 with the ATLAS detector at the Large Hadron Collider in
proton-proton collisions at . One event satisfying the
signal selection criteria is observed, which is consistent
with the expected background rate. Limits on the product of
the WH production cross section and the branching ratio of a
Higgs boson decaying to prompt electron-jets are calculated
as a function of a Higgs boson mass in the range from 100 to
140 GeV. © CERN 2013 for the benefit of the ATLAS
Collaboration, published under the terms of the Creative
Commons Attribution 3.0 licence by IOP Publishing Ltd and
Deutsche Physikalische Gesellschaft. Any further
distribution of this work must maintain attribution to the
author(s) and the published article's title, journal
citation and DOI.},
Doi = {10.1088/1367-2630/15/4/043009},
Key = {fds307605}
}
@article{fds307995,
Author = {Aaltonen, T and others},
Title = {Search for WW and WZ production in lepton plus jets final
state at CDF},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {11},
Pages = {112011},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.112011},
Abstract = {We present a search for WW and WZ production in final states
that contain a charged lepton (electron or muon) and at
least two jets, produced in sqrt[s]=1.96 TeV pp̅
collisions at the Fermilab Tevatron, using data
corresponding to 1.2 fb-1 of integrated luminosity
collected with the CDF II detector. Diboson production in
this decay channel has yet to be observed at hadron
colliders due to the large single W plus jets background. An
artificial neural network has been developed to increase
signal sensitivity, as compared with an event selection
based on conventional cuts. We set a 95% confidence level
upper limit of σWW×BR(W→ℓνℓ,W→jets)+σWZ×BR(W→ℓνℓ,Z→jets)<2.88 pb,
which is consistent with the standard model
next-to-leading-order cross section calculation for this
decay channel of 2.09 ± 0.12 pb.},
Doi = {10.1103/PhysRevD.79.112011},
Key = {fds307995}
}
@article{fds310351,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Search for WZ resonances in the fully leptonic channel using
pp collisions at s=8 TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {737},
Pages = {223-243},
Publisher = {Elsevier BV},
Year = {2014},
Month = {October},
url = {http://dx.doi.org/10.1016/j.physletb.2014.08.039},
Abstract = {A search for resonant WZ production in the ℓνℓ'ℓ'
(ℓ,ℓ'=e,μ) decay channel using 20.3 fb-1 of s=8TeV pp
collision data collected by the ATLAS experiment at LHC is
presented. No significant deviation from the Standard Model
prediction is observed and upper limits on the production
cross sections of WZ resonances from an extended gauge model
W' and from a simplified model of heavy vector triplets are
derived. A corresponding observed (expected) lower mass
limit of 1.52 (1.49) TeV is derived for the W' at the 95%
confidence level. © 2014 Elsevier B.V.},
Doi = {10.1016/j.physletb.2014.08.039},
Key = {fds310351}
}
@article{fds307806,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett,
W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd,
HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito,
L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli,
M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca almenar, C and Cuevas, J and Culbertson, R and Dagenhart, D},
Title = {Search for WZ+ZZ production with missing transverse
energy+jets with b enhancement at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.85.012002},
Abstract = {Diboson production (WW+WZ+ZZ) has been observed at the
Tevatron in hadronic decay modes dominated by the WW
process. This paper describes the measurement of the cross
section of WZ and ZZ events in final states with large E T
and using b-jet identification as a tool to suppress WW
contributions. Because of the limited energy resolution, we
cannot distinguish between partially hadronic decays of WZ
and ZZ, and we measure the sum of these processes. The
number of signal events is extracted using a simultaneous
fit to the invariant mass distribution of the two jets for
events with two b-jet candidates and events with fewer than
two b-jet candidates. We measure a cross section
σ(pp̄→WZ,ZZ)=5.8-3.0+3.6pb, in agreement with the
standard model. © 2012 American Physical
Society.},
Doi = {10.1103/PhysRevD.85.012002},
Key = {fds307806}
}
@article{fds356679,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik,
Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli,
E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aperio
Bella, L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz,
V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Search for W′ → tb decays in the hadronic final
state using pp collisions at √s=13TeV with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {781},
Pages = {327-348},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1016/j.physletb.2018.03.036},
Abstract = {A search for W′-boson production in the
W′→tb¯→qq¯′bb¯ decay channel is presented using
36.1fb−1 of 13 TeV proton–proton collision data
collected by the ATLAS detector at the Large Hadron Collider
in 2015 and 2016. The search is interpreted in terms of both
a left-handed and a right-handed chiral W′ boson within
the mass range 1–5 TeV. Identification of the hadronically
decaying top quark is performed using jet substructure
tagging techniques based on a shower deconstruction
algorithm. No significant deviation from the Standard Model
prediction is observed and the results are expressed as
upper limits on the W′→tb¯ production cross-section
times branching ratio as a function of the W′-boson mass.
These limits exclude W′ bosons with right-handed couplings
with masses below 3.0 TeV and W′ bosons with left-handed
couplings with masses below 2.9 TeV, at the 95% confidence
level.},
Doi = {10.1016/j.physletb.2018.03.036},
Key = {fds356679}
}
@article{fds308140,
Author = {Acosta, D and Adelman, J and Affolder, T and Akimoto, T and Albrow, MG and Ambrose, D and Amerio, S and Amidei, D and Anastassov, A and Anikeev, K and Annovi, A and Antos, J and Aoki, M and Apollinari, G and Arisawa, T and Arguin, JF and Artikov, A and Ashmanskas, W and Attal, A and Azfar, F and Azzi-Bacchetta, P and Bacchetta, N and Bachacou, H and Badgett, W and Barbaro-Galtieri, A and Barker, GJ and Barnes, VE and Barnett, BA and Baroiant, S and Barone, M and Bauer, G and Bedeschi, F and Behari, S and Belforte, S and Bellettini, G and Bellinger, J and Ben-Haim, E and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bishai, M and Blair, RE and Blocker, C and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Bolla, G and Bolshov, A and Booth, PSL and Bortoletto, D and Boudreau, J and Bourov, S and Brau, B and Bromberg, C and Brubaker, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Byrum, KL and Cabrera, S and Campanelli, M and Campbell,
M and Canepa, A and Casarsa, M and Carlsmith, D and Carron, S and Carosi,
R and Cavalli-Sforza, M and Castro, A and Catastini, P and Cauz, D and Cerri, A and Cerrito, L and Chapman, J and Chen, C and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
I and Cho, K and Chokheli, D and Chou, JP and Chu, ML and Chuang, S and Chung,
JY and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark,
AG and Clark, D and Coca, M and Connolly, A},
Title = {Search for ZZ and ZW production in pp̄ collisions at
s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {71},
Number = {9},
Pages = {1-7},
Publisher = {American Physical Society (APS)},
Year = {2005},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.71.091105},
Abstract = {We present a search for ZZ and ZW vector boson pair
production in pp̄ collisions at s=1.96TeV using the
leptonic decay channels ZZ→llνν, ZZ→lll′l′, and
ZW→lll′ν. In a data sample corresponding to an
integrated luminosity of 194pb-1 collected with the Collider
Detector at Fermilab, 3 candidate events are found with an
expected background of 1.0±0.2 events. We set a 95%
confidence level upper limit of 15.2pb on the cross section
for ZZ plus ZW production, compared to the standard model
prediction of 5.0±0.4pb. © 2005 The American Physical
Society.},
Doi = {10.1103/PhysRevD.71.091105},
Key = {fds308140}
}
@article{fds310321,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel
Khalek, S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, A and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, K and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow,
TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer,
J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Buehrer,
F and Bugge, L and Bugge, MK and Bulekov, O and Bundock, AC and Burckhart,
H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Buszello,
CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere, V and Cavalli,
D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, B and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Search for [Formula: see text] decays in [Formula: see text]
collisions at [Formula: see text] = 8 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {4},
Pages = {165},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3372-2},
Abstract = {A search for a massive [Formula: see text] gauge boson
decaying to a top quark and a bottom quark is performed with
the ATLAS detector in [Formula: see text] collisions at the
LHC. The dataset was taken at a centre-of-mass energy of
[Formula: see text] and corresponds to [Formula: see text]
of integrated luminosity. This analysis is done in the
hadronic decay mode of the top quark, where novel jet
substructure techniques are used to identify jets from
high-momentum top quarks. This allows for a search for
high-mass [Formula: see text] bosons in the range
1.5-3.0 [Formula: see text]. [Formula: see text]-tagging is
used to identify jets originating from [Formula: see
text]-quarks. The data are consistent with Standard Model
background-only expectations, and upper limits at 95 %
confidence level are set on the [Formula: see text] cross
section times branching ratio ranging from [Formula: see
text] to [Formula: see text] for left-handed [Formula: see
text] bosons, and ranging from [Formula: see text] to
[Formula: see text] for [Formula: see text] bosons with
purely right-handed couplings. Upper limits at 95 %
confidence level are set on the [Formula: see text]-boson
coupling to [Formula: see text] as a function of the
[Formula: see text] mass using an effective field theory
approach, which is independent of details of particular
models predicting a [Formula: see text] boson.},
Doi = {10.1140/epjc/s10052-015-3372-2},
Key = {fds310321}
}
@article{fds307880,
Author = {Aaltonen, and T, and al, E},
Title = {Search for {Randall-Sundrum} gravitons in the diphoton
channel at {CDF}},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {1},
Pages = {011102},
Publisher = {American Physical Society},
Year = {2011},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.83.011102},
Abstract = {We report on a search for new particles in the diphoton
channel using a data sample of pp̄ collisions at
√s=1.96TeV collected by the CDF II detector at the
Fermilab Tevatron, with an integrated luminosity of
5.4fb⊃-1. The diphoton invariant mass spectrum of the data
agrees well with the standard model expectation. We set
upper limits on the production cross section times branching
ratio for the Randall-Sundrum graviton, as a function of
diphoton mass. We subsequently derive lower limits on the
graviton mass of 459GeV/c2 and 963GeV/c2, at the 95%
confidence level, for coupling parameters (k/M̄Pl) of 0.01
and 0.1, respectively. © 2011 American Physical
Society.},
Doi = {10.1103/PhysRevD.83.011102},
Key = {fds307880}
}
@article{fds373467,
Author = {Amerl, M and Filmer, EK and Jackson, P and Kong, AXY and Potti, H and Ruggeri, TA and Ting, EXL and White, MJ and Gingrich, DM and Lindon, JH and Nishu, N and Pinfold, JL and Cakir, O and Yildiz, HD and Kuday, S and Turk
Cakir, I and Sultansoy, S and Adam Bourdarios and C and Berger, N and Costanza, F and Delmastro, M and Di Ciaccio and L and Goy, C and Guillemin,
T and Hryn’ova, T and Jézéquel, S and Koletsou, I and Levêque, J and Lewis, DJ and Little, JD and Lorenzo Martinez and N and Poddar, G and Rossi, E and Sanchez Pineda and A and Sauvan, E and Selem, L and Bernardi,
G and Bomben, M and Bouquet, R and Di Gregorio and G and Li, A and Marchiori,
G and Shen, Q and Zhang, Y and Chekanov, S and Darmora, S and Hopkins, WH and Hoya, J and Kourlitis, E and LeCompte, T and Love, J and Metcalfe, J and Mete, AS and Paramonov, A and Proudfoot, J and Van Gemmeren and P and Wang,
R and Zhang, J and Berlendis, S and Cheu, E and Cui, Z and Ghosh, A and Johns,
KA and Lampl, W and Lindley, RE and Loch, P and Rutherfoord, JP and Sardain, J and Varnes, EW and Zhou, H and Zhou, Y and Bakshi Gupta and D and Burghgrave, B and Cardenas, JCJ and De, K and Farbin, A and Hadavand,
HK and Myers, AJ and Ozturk, N and Usai, G and White, A and Angelidakis, S and Fassouliotis, D and Fountas, L and Gkialas, I and Kourkoumelis, C and Alexopoulos, T and Bakalis, C and Drivas-Koulouris, I and Gazis, EN and Kitsaki, C and Maltezos, S and Paraskevopoulos, C and Perganti, M and Tzanis, P and Andeen, T and Burton, CD and Choi, K and Onyisi, PUE and Panchal, DK},
Title = {Search in diphoton and dielectron final states for displaced
production of Higgs or Z bosons with the ATLAS detector in
Formula Presented pp collisions},
Journal = {Physical Review D},
Volume = {108},
Number = {1},
Year = {2023},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.108.012012},
Abstract = {A search is presented for displaced production of Higgs
bosons or Z bosons, originating from the decay of a neutral
long-lived particle (LLP) and reconstructed in the decay
modes H → γ γ and Z → e e . The analysis uses the full
Run 2 dataset of proton-proton collisions delivered by the
LHC at an energy of s = 13 TeV between 2015 and 2018 and
recorded by the ATLAS detector, corresponding to an
integrated luminosity of 139 fb - 1 . Exploiting the
capabilities of the ATLAS liquid argon calorimeter to
precisely measure the arrival times and trajectories of
electromagnetic objects, the analysis searches for the
signature of pairs of photons or electrons which arise from
a common displaced vertex and which arrive after some delay
at the calorimeter. The results are interpreted in a
gauge-mediated supersymmetry breaking model with
pair-produced Higgsinos that decay to LLPs, and each LLP
subsequently decays into either a Higgs boson or a Z boson.
The final state includes at least two particles that escape
direct detection, giving rise to missing transverse
momentum. No significant excess is observed above the
background expectation. The results are used to set upper
limits on the cross section for Higgsino pair production, up
to a χ ˜ 1 0 mass of 369 (704) GeV for decays with 100%
branching ratio of χ ˜ 1 0 to Higgs ( Z ) bosons for a χ
˜ 1 0 lifetime of 2 ns. A model-independent limit is also
set on the production of pairs of photons or electrons with
a significant delay in arrival at the calorimeter.},
Doi = {10.1103/PhysRevD.108.012012},
Key = {fds373467}
}
@article{fds308065,
Author = {Aaltonen, T and others},
Title = {Searches for direct pair production of supersymmetric top
and supersymmetric bottom quarks in p[overline p] collisions
at $\sqrt{s}$=1.96 TeV},
Journal = {Phys. Rev.},
Volume = {D76},
Number = {7},
Pages = {072010},
Publisher = {American Physical Society (APS)},
Year = {2007},
url = {http://dx.doi.org/10.1103/PhysRevD.76.072010},
Abstract = {We search for direct pair production of supersymmetric top
quarks and supersymmetric bottom quarks in proton-antiproton
collisions at sqrt(s)=1.96 TeV, using 295 pb-1 of data
recorded by the Collider Detector at Fermilab (CDF II)
experiment. The supersymmetric top (supersymmetric bottom)
quarks are selected by reconstructing their decay into a
charm (bottom) quark and a neutralino, which is assumed to
be the lightest supersymmetric particle. The signature of
such processes is two energetic heavy-flavor jets and
missing transverse energy. The number of events that pass
our selection for each search process is consistent with the
expected standard model background. By comparing our results
to the theoretical production cross sections of the
supersymmetric top and supersymmetric bottom quarks in the
minimal supersymmetric standard model, we exclude, at a 95%
confidence level in the frame of that model, a
supersymmetric top quark mass up to 132 GeV/c2 for a
neutralino mass of 48 GeV/c2, and a supersymmetric bottom
quark mass up to 193 GeV/c2 for a neutralino mass of 40
GeV/c2.},
Doi = {10.1103/PhysRevD.76.072010},
Key = {fds308065}
}
@article{fds349429,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH and Arduh, FA},
Title = {Searches for electroweak production of supersymmetric
particles with compressed mass spectra in s =13 TeV pp
collisions with the ATLAS detector},
Journal = {Physical Review D},
Volume = {101},
Number = {5},
Year = {2020},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.101.052005},
Abstract = {This paper presents results of searches for the electroweak
production of supersymmetric particles in models with
compressed mass spectra. The searches use 139 fb-1 of s=13
TeV proton-proton collision data collected by the ATLAS
experiment at the Large Hadron Collider. Events with missing
transverse momentum and two same-flavor, oppositely charged,
low-transverse-momentum leptons are selected, and are
further categorized by the presence of hadronic activity
from initial-state radiation or a topology compatible with
vector-boson fusion processes. The data are found to be
consistent with predictions from the Standard Model. The
results are interpreted using simplified models of
R-parity-conserving supersymmetry in which the lightest
supersymmetric partner is a neutralino with a mass similar
to the lightest chargino, the second-to-lightest neutralino,
or the slepton. Lower limits on the masses of charginos in
different simplified models range from 193 to 240 GeV for
moderate mass splittings, and extend down to mass splittings
of 1.5 to 2.4 GeV at the LEP chargino bounds (92.4 GeV).
Similar lower limits on degenerate light-flavor sleptons
extend up to masses of 251 GeV and down to mass splittings
of 550 MeV. Constraints on vector-boson fusion production of
electroweak SUSY states are also presented.},
Doi = {10.1103/PhysRevD.101.052005},
Key = {fds349429}
}
@article{fds372743,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel,
A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Amelung, C and Ames,
CG and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche,
CS and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Pozo, JAA and Aparo, MA and Bella, LA and Appelt, C and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce, ATH and Arena,
E},
Title = {Searches for exclusive Higgs and Z boson decays into a
vector quarkonium state and a photon using 139 fb -
1 of ATLAS √s=13 TeV proton–proton collision
data},
Journal = {European Physical Journal C},
Volume = {83},
Number = {9},
Year = {2023},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11869-1},
Abstract = {Searches for the exclusive decays of Higgs and Z bosons into
a vector quarkonium state and a photon are performed in the
μ+μ-γ final state with a proton–proton collision data
sample corresponding to an integrated luminosity of 139 fb
- 1 collected at s=13 TeV with the ATLAS detector at the
CERN Large Hadron Collider. The observed data are compatible
with the expected backgrounds. The 95% confidence-level
upper limits on the branching fractions of the Higgs boson
decays into J/ψγ , ψ(2S)γ , and Υ(1S,2S,3S)γ are found
to be 2.0 × 10 - 4 , 10.5 × 10 - 4 , and (2.5 , 4.2 , 3.4)
× 10 - 4 , respectively, assuming Standard Model production
of the Higgs boson. The corresponding 95% CL upper limits on
the branching fractions of the Z boson decays are 1.2 × 10
- 6 , 2.4 × 10 - 6 , and (1.1 , 1.3 , 2.4) × 10 - 6 . An
observed 95% CL interval of (- 133 , 175) is obtained for
the κc/ κγ ratio of Higgs boson coupling modifiers, and a
95% CL interval of (- 37 , 40) is obtained for κb/ κγ
.},
Doi = {10.1140/epjc/s10052-023-11869-1},
Key = {fds372743}
}
@article{fds356639,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Searches for exclusive Higgs and Z boson decays into
J/ψ γ, ψ(2S) γ, and ϒ(nS) γ at s=13TeV with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {786},
Pages = {134-155},
Year = {2018},
Month = {November},
url = {http://dx.doi.org/10.1016/j.physletb.2018.09.024},
Abstract = {Searches for the exclusive decays of the Higgs and Z bosons
into a J/ψ, ψ(2S), or ϒ(nS) (n=1,2,3) meson and a photon
are performed with a pp collision data sample corresponding
to an integrated luminosity of 36.1fb−1 collected at
s=13TeV with the ATLAS detector at the CERN Large Hadron
Collider. No significant excess of events is observed above
the expected backgrounds, and 95% confidence-level upper
limits on the branching fractions of the Higgs boson decays
to J/ψγ, ψ(2S)γ, and ϒ(nS)γ of 3.5×10−4,
2.0×10−3, and (4.9,5.9,5.7)×10−4, respectively, are
obtained assuming Standard Model production. The
corresponding 95% confidence-level upper limits for the
branching fractions of the Z boson decays are 2.3×10−6,
4.5×10−6 and (2.8,1.7,4.8)×10−6, respectively.},
Doi = {10.1016/j.physletb.2018.09.024},
Key = {fds356639}
}
@article{fds321097,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez
Gonzalez, B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor
Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella,
L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Searches for heavy diboson resonances in pp collisions at
√s=13 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {9},
Publisher = {Springer Nature},
Year = {2016},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2016)173},
Abstract = {Searches for new heavy resonances decaying to WW, WZ, and ZZ
bosons are presented, using a data sample corresponding to
3.2 fb−1 of pp collisions at s=13 TeV collected with the
ATLAS detector at the CERN Large Hadron Collider. Analyses
selecting ννqq, ℓνqq, ℓℓqq and qqqq final states
are combined, searching for an arrow-width resonance with
mass between 500 and 3000 GeV. The discriminating variable
is either an invariant mass or a transverse mass. No
significant deviations from the Standard Model predictions
are observed. Three benchmark models are tested: a model
predicting the existence of a new heavy scalar singlet, a
simplified model predicting a heavy vector-boson triplet,
and a bulk Randall-Sundrum model with a heavy spin-2
graviton. Cross-section limits are set at the 95% confidence
level and are compared to theoretical cross-section
predictions for a variety of models. The data exclude a
scalar singlet with mass below 2650 GeV, a heavy
vector-boson triplet with mass below 2600 GeV, and a
graviton with mass below 1100 GeV. These results
significantly extend the previous limits set using pp
collisions at s=8 TeV.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP09(2016)173},
Key = {fds321097}
}
@article{fds310329,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti,
Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit,
S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert,
J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O},
Title = {Searches for heavy long-lived charged particles with the
ATLAS detector in proton-proton collisions at √s = 8
Tev},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {1},
Publisher = {Springer Nature},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1007/JHEP01(2015)068},
Abstract = {Abstract: Searches for heavy long-lived charged particles
are performed using a data sample of 19.1 fb−1 from
proton-proton collisions at a centre-of-mass energy of s=8$$
\sqrt{s}=8 $$ TeV collected by the ATLAS detector at the
Large Hadron Collider. No excess is observed above the
estimated background and limits are placed on the mass of
long-lived particles in various supersymmetric models.
Long-lived tau sleptons in models with gauge-mediated
symmetry breaking are excluded up to masses between 440 and
385 GeV for tan β between 10 and 50, with a 290 GeV limit
in the case where only direct tau slepton production is
considered. In the context of simplified LeptoSUSY models,
where sleptons are stable and have a mass of 300 GeV, squark
and gluino masses are excluded up to a mass of 1500 and 1360
GeV, respectively. Directly produced charginos, in
simplified models where they are nearly degenerate to the
lightest neutralino, are excluded up to a mass of 620 GeV.
R-hadrons, composites containing a gluino, bottom squark or
top squark, are excluded up to a mass of 1270, 845 and 900
GeV, respectively, using the full detector; and up to a mass
of 1260, 835 and 870 GeV using an approach disregarding
information from the muon spectrometer.[Figure not
available: see fulltext.]},
Doi = {10.1007/JHEP01(2015)068},
Key = {fds310329}
}
@article{fds356790,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M},
Title = {Searches for heavy long-lived sleptons and R-hadrons with
the ATLAS detector in pp collisions at √s=7
TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {720},
Number = {4-5},
Pages = {277-308},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2013.02.015},
Abstract = {A search for long-lived particles is performed using a data
sample of 4.7 fb−1 from proton–proton collisions at a
centre-of-mass energy s=7 TeV collected by the ATLAS
detector at the LHC. No excess is observed above the
estimated background and lower limits, at 95% confidence
level, are set on the mass of the long-lived particles in
different scenarios, based on their possible interactions in
the inner detector, the calorimeters and the muon
spectrometer. Long-lived staus in gauge-mediated
SUSY-breaking models are excluded up to a mass of 300 GeV
for tanβ=5–20. Directly produced long-lived sleptons are
excluded up to a mass of 278 GeV. R-hadrons, composites of
gluino (stop, sbottom) and light quarks, are excluded up to
a mass of 985 GeV (683 GeV, 612 GeV) when using a generic
interaction model. Additionally two sets of limits on
R-hadrons are obtained that are less sensitive to the
interaction model for R-hadrons. One set of limits is
obtained using only the inner detector and calorimeter
observables, and a second set of limits is obtained based on
the inner detector alone.},
Doi = {10.1016/j.physletb.2013.02.015},
Key = {fds356790}
}
@article{fds356692,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Searches for heavy ZZ and ZW resonances in the ℓℓqq and
ννqq final states in pp collisions at √s=13 TeV with the
ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2018},
Number = {3},
Year = {2018},
Month = {March},
url = {http://dx.doi.org/10.1007/JHEP03(2018)009},
Abstract = {This paper reports searches for heavy resonances decaying
into ZZ or ZW using data from proton-proton collisions at a
centre-of-mass energy of s=13 TeV. The data, corresponding
to an integrated luminosity of 36.1 fb−1, were recorded
with the ATLAS detector in 2015 and 2016 at the Large Hadron
Collider. The searches are performed in final states in
which one Z boson decays into either a pair of light charged
leptons (electrons and muons) or a pair of neutrinos, and
the associated W boson or the other Z boson decays
hadronically. No evidence of the production of heavy
resonances is observed. Upper bounds on the production cross
sections of heavy resonances times their decay branching
ratios to ZZ or ZW are derived in the mass range 300-5000GeV
within the context of Standard Model extensions with
additional Higgs bosons, a heavy vector triplet or warped
extra dimensions. Production through gluon-gluon fusion,
Drell-Yan or vector-boson fusion are considered, depending
on the assumed model.[Figure not available: see
fulltext.].},
Doi = {10.1007/JHEP03(2018)009},
Key = {fds356692}
}
@article{fds356544,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali,
B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez,
M and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza,
A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio
Bella, L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo
Pereira, R},
Title = {Searches for lepton-flavour-violating decays of the Higgs
boson in s=13 TeV pp collisions with the ATLAS
detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {800},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2019.135069},
Abstract = {This Letter presents direct searches for lepton flavour
violation in Higgs boson decays, H→eτ and H→μτ,
performed with the ATLAS detector at the LHC. The searches
are based on a data sample of proton–proton collisions at
a centre-of-mass energy s=13 TeV, corresponding to an
integrated luminosity of 36.1 fb−1. No significant excess
is observed above the expected background from Standard
Model processes. The observed (median expected) 95%
confidence-level upper limits on the lepton-flavour-violating
branching ratios are 0.47% (0.34−0.10+0.13%) and 0.28%
(0.37−0.10+0.14%) for H→eτ and H→μτ,
respectively.},
Doi = {10.1016/j.physletb.2019.135069},
Key = {fds356544}
}
@article{fds372389,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Hoffman, ACA and Acharya, BS and Achkar, B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Addepalli,
SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder,
AA and Afik, Y and Agapopoulou, C and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad,
A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Arcangeletti, C and Arce,
ATH},
Title = {Searches for new phenomena in events with two leptons, jets,
and missing transverse momentum in 139 fb - 1 of
√s=13 TeV pp collisions with the ATLAS
detector},
Journal = {European Physical Journal C},
Volume = {83},
Number = {6},
Year = {2023},
Month = {June},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11434-w},
Abstract = {Searches for new phenomena inspired by supersymmetry in
final states containing an e+e- or μ+μ- pair, jets, and
missing transverse momentum are presented. These searches
make use of proton–proton collision data with an
integrated luminosity of 139fb-1 , collected during
2015–2018 at a centre-of-mass energy s=13 TeV by the ATLAS
detector at the Large Hadron Collider. Two searches target
the pair production of charginos and neutralinos. One uses
the recursive-jigsaw reconstruction technique to follow up
on excesses observed in 36.1fb-1 of data, and the other uses
conventional event variables. The third search targets pair
production of coloured supersymmetric particles (squarks or
gluinos) decaying through the next-to-lightest neutralino
(χ~20) via a slepton (ℓ~) or Z boson into ℓ+ℓ-χ~10 ,
resulting in a kinematic endpoint or peak in the dilepton
invariant mass spectrum. The data are found to be consistent
with the Standard Model expectations. Results are
interpreted using simplified models and exclude masses up to
900 GeV for electroweakinos, 1550 GeV for squarks, and
2250 GeV for gluinos.},
Doi = {10.1140/epjc/s10052-023-11434-w},
Key = {fds372389}
}
@article{fds356578,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi
Pozo, JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo
Ferraz, V and Araujo Pereira and R and Arce, ATH and Ardell, RE and Arduh,
FA and Arguin, JF and Argyropoulos, S and Armbruster, AJ and Armitage,
LJ and Armstrong, A and Arnaez, O},
Title = {Searches for scalar leptoquarks and differential
cross-section measurements in dilepton–dijet events in
proton–proton collisions at a centre-of-mass energy of
√s = 13 TeV with the ATLAS experiment},
Journal = {European Physical Journal C},
Volume = {79},
Number = {9},
Year = {2019},
Month = {September},
url = {http://dx.doi.org/10.1140/epjc/s10052-019-7181-x},
Abstract = {Searches for scalar leptoquarks pair-produced in
proton–proton collisions at s=13 TeV at the Large Hadron
Collider are performed by the ATLAS experiment. A data set
corresponding to an integrated luminosity of 36.1 fb- 1 is
used. Final states containing two electrons or two muons and
two or more jets are studied, as are states with one
electron or muon, missing transverse momentum and two or
more jets. No statistically significant excess above the
Standard Model expectation is observed. The observed and
expected lower limits on the leptoquark mass at 95%
confidence level extend up to 1.29 TeV and 1.23 TeV for
first- and second-generation leptoquarks, respectively, as
postulated in the minimal Buchmüller–Rückl–Wyler
model, assuming a branching ratio into a charged lepton and
a quark of 50%. In addition, measurements of particle-level
fiducial and differential cross sections are presented for
the Z→ ee, Z→ μμ and tt¯ processes in several regions
related to the search control regions. Predictions from a
range of generators are compared with the measurements, and
good agreement is seen for many of the observables. However,
the predictions for the Z→ ℓℓ measurements in
observables sensitive to jet energies disagree with the
data.},
Doi = {10.1140/epjc/s10052-019-7181-x},
Key = {fds356578}
}
@article{fds321130,
Author = {ATLAS Collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann,
TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti,
M and Bilbao De Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard,
J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta,
SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos,
K and Boscherini, D and Bosman, M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden,
WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger,
D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni,
A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes,
T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and CabreraUrbán, S and Caforio, D and Cairo, VM and Cakir, O and Calace,
N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano
Bret, M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido,
MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau,
CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn, AP},
Title = {Searches for scalar leptoquarks in pp collisions at
[Formula: see text] = 8 TeV with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {5},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3823-9},
Abstract = {Searches for pair-produced scalar leptoquarks are performed
using 20 fb[Formula: see text] of proton-proton collision
data provided by the LHC and recorded by the ATLAS detector
at [Formula: see text] TeV. Events with two electrons
(muons) and two or more jets in the final state are used to
search for first (second)-generation leptoquarks. The
results from two previously published ATLAS analyses are
interpreted in terms of third-generation leptoquarks
decaying to [Formula: see text] and [Formula: see text]
final states. No statistically significant excess above the
Standard Model expectation is observed in any channel and
scalar leptoquarks are excluded at 95 % CL with masses up
to [Formula: see text] 1050 GeV for first-generation
leptoquarks, [Formula: see text] 1000 GeV for
second-generation leptoquarks, [Formula: see text] 625 GeV
for third-generation leptoquarks in the [Formula: see
text] channel, and 200 [Formula: see text] 640 GeV in
the [Formula: see text] channel.},
Doi = {10.1140/epjc/s10052-015-3823-9},
Key = {fds321130}
}
@article{fds307760,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault,
JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster,
AJ and Arnaez, O and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D},
Title = {Searches for supersymmetry with the ATLAS detector using
final states with two leptons and missing transverse
momentum in s=7TeV proton-proton collisions},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {709},
Number = {3},
Pages = {137-157},
Publisher = {Elsevier BV},
Year = {2012},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2012.01.076},
Abstract = {Results of three searches are presented for the production
of supersymmetric particles decaying into final states with
missing transverse momentum and exactly two isolated
leptons, e or μ. The analysis uses a data sample collected
during the first half of 2011 that corresponds to a total
integrated luminosity of 1fb-1 of s=7TeV proton-proton
collisions recorded with the ATLAS detector at the Large
Hadron Collider. Opposite-sign and same-sign dilepton events
are separately studied, with no deviations from the Standard
Model expectation observed. Additionally, in opposite-sign
events, a search is made for an excess of same-flavour over
different-flavour lepton pairs. Effective production cross
sections in excess of 9.9 fb for opposite-sign events
containing supersymmetric particles with missing transverse
momentum greater than 250 GeV are excluded at 95% CL. For
same-sign events containing supersymmetric particles with
missing transverse momentum greater than 100 GeV, effective
production cross sections in excess of 14.8 fb are excluded
at 95% CL. The latter limit is interpreted in a simplified
electroweak gaugino production model excluding chargino
masses up to 200 GeV, under the assumption that slepton
decay is dominant. © 2012 CERN.},
Doi = {10.1016/j.physletb.2012.01.076},
Key = {fds307760}
}
@article{fds307579,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bertoli, G and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Canepa, A and Carls, B and Carlsmith, D and Carosi, R and Carrillo,
S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen,
YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci, MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo,
N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza and B and Dittmann,
JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina,
K},
Title = {Searches for the Higgs boson decaying to W+W
-→ℓ+νℓ-ν̄ with the
CDF II detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.88.052012},
Abstract = {We present a search for a standard model Higgs boson
decaying to two W bosons that decay to leptons using the
full data set collected with the CDF II detector in
√s=1.96 TeV pp̄ collisions at the Fermilab Tevatron,
corresponding to an integrated luminosity of 9.7 fb-1. We
obtain no evidence for production of a standard model Higgs
boson with mass between 110 and 200 GeV/c2, and place upper
limits on the production cross section within this range. We
exclude standard model Higgs boson production at the 95%
confidence level in the mass range between 149 and 172
GeV/c2, while expecting to exclude, in the absence of
signal, the range between 155 and 175 GeV/c2. We also
interpret the search in terms of standard model Higgs boson
production in the presence of a fourth generation of
fermions and within the context of a fermiophobic Higgs
boson model. For the specific case of a standard-model-like
Higgs boson in the presence of fourth-generation fermions,
we exclude at the 95% confidence level Higgs boson
production in the mass range between 124 and 200 GeV/c2,
while expecting to exclude, in the absence of signal, the
range between 124 and 221 GeV/c2. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.052012},
Key = {fds307579}
}
@article{fds356731,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Searches for the Zγ decay mode of the Higgs boson and for
new high-mass resonances in pp collisions at √s=13 TeV
with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {10},
Year = {2017},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2017)112},
Abstract = {This article presents searches for the Zγ decay of the
Higgs boson and for narrow high-mass resonances decaying to
Zγ, exploiting Z boson decays to pairs of electrons or
muons. The data analysis uses 36.1 fb−1 of pp collisions
at s=13 recorded by the ATLAS detector at the CERN Large
Hadron Collider. The data are found to be consistent with
the expected Standard Model background. The observed
(expected — assuming Standard Model pp → H → Zγ
production and decay) upper limit on the production cross
section times the branching ratio for pp → H → Zγ is
6.6. (5.2) times the Standard Model prediction at the 95%
confidence level for a Higgs boson mass of 125.09 GeV. In
addition, upper limits are set on the production cross
section times the branching ratio as a function of the mass
of a narrow resonance between 250 GeV and 2.4 TeV, assuming
spin-0 resonances produced via gluon-gluon fusion, and
spin-2 resonances produced via gluon-gluon or
quark-antiquark initial states. For high-mass spin-0
resonances, the observed (expected) limits vary between 88
fb (61 fb) and 2.8 fb (2.7 fb) for the mass range from 250
GeV to 2.4 TeV at the 95% confidence level.},
Doi = {10.1007/JHEP10(2017)112},
Key = {fds356731}
}
@article{fds356595,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger,
M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agapopoulou,
C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Estevez and M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Arduh, FA and Arguin, JF},
Title = {Searches for third-generation scalar leptoquarks in √s =
13 TeV pp collisions with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {6},
Year = {2019},
Month = {June},
url = {http://dx.doi.org/10.1007/JHEP06(2019)144},
Abstract = {Limits are set on the pair production of scalar leptoquarks,
where all possible decays of the leptoquark into a quark (t,
b) and a lepton (τ, ν) of the third generation are
considered. The limits are presented as a function of the
leptoquark mass and the branching ratio into charged leptons
for up-type (LQ3u → tν/bτ) and down-type (LQ3d →
bν/tτ) leptoquarks. Many results are reinterpretations of
previously published ATLAS searches. In all cases, LHC
proton-proton collision data at a centre-of-mass energy of s
= 13 TeV recorded by the ATLAS detector in 2015 and 2016 are
used, corresponding to an integrated luminosity of 36.1
fb−1. Masses below 800 GeV are excluded for both LQ3u and
LQ3d independently of the branching ratio, with masses below
about 1 TeV being excluded for the limiting cases of
branching ratios equal to zero or unity.[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP06(2019)144},
Key = {fds356595}
}
@article{fds359268,
Author = {Kotwal, AV},
Title = {Searching for metastable particles using graph
computing.},
Journal = {Scientific reports},
Volume = {11},
Number = {1},
Pages = {18543},
Year = {2021},
Month = {September},
url = {http://dx.doi.org/10.1038/s41598-021-97848-6},
Abstract = {The reconstruction of charged particle trajectories at the
Large Hadron Collider and future colliders relies on energy
depositions in sensors placed at distances ranging from a
centimeter to a meter from the colliding beams. We propose a
method of detecting charged particles that decay invisibly
after traversing a short distance of about 25 cm inside the
experimental apparatus. One of the decay products may
constitute the dark matter known to be 84% of all matter at
galactic and cosmological distance scales. Our method uses
graph computing to cluster spacepoints recorded by
two-dimensional silicon pixel sensors into
mathematically-defined patterns. The algorithm may be
implemented on silicon-based integrated circuits using
field-programmable gate array technology to augment or
replace traditional computing platforms.},
Doi = {10.1038/s41598-021-97848-6},
Key = {fds359268}
}
@article{fds307986,
Author = {Aaltonen, T and others},
Title = {Searching the inclusive ℓγE̸T+b-quark signature for
radiative top quark decay and non-standard-model
processes},
Journal = {Phys. Rev. D},
Volume = {80},
Number = {1},
Pages = {011102},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.80.011102},
Abstract = {We compare the inclusive production of events containing a
lepton (ℓ), a photon (γ), significant transverse momentum
imbalance (E̸T), and a jet identified as containing a
b-quark, to SM predictions. The search uses data produced in
proton-antiproton collisions at sqrt[s]=1.96 TeV
corresponding to 1.9 fb-1 of integrated luminosity
taken with the CDF detector. We find 28 ℓγbE̸T events
versus an expectation of 31.0-3.5+4.1 events. If we further
require events to contain at least three jets and large
total transverse energy, the largest SM source is radiative
top-quark pair production, tt̅ +γ. In the data we observe
16 tt̅ γ candidate events versus an expectation from SM
sources of 11.2-2.1+2.3. Assuming the difference between the
observed number and the predicted non-top-quark total of
6.8-2.0+2.2 is due to SM top-quark production, we estimate
the tt̅ γ cross section to be 0.15 ±
0.08 pb.},
Doi = {10.1103/PhysRevD.80.011102},
Key = {fds307986}
}
@article{fds310307,
Author = {Auerbach, B and Chekanov, S and Love, J and Proudfoot, J and Kotwal,
AV},
Title = {Sensitivity to new high-mass states decaying to tt¯ at a
100 TeV collider},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.91.034014},
Abstract = {We discuss the sensitivity of a 100 TeV pp collider to heavy
particles decaying to top-antitop (tt¯) final states. This
center-of-mass energy, together with an integrated
luminosity of 10ab-1, can produce heavy particles in the
mass range of several tens of teraelectronvolts (TeV). A
Monte Carlo study is performed using boosted-top techniques
to reduce QCD background for the reconstruction of heavy
particles with masses in the range of 8-20 TeV, and various
widths. In particular, we study two models that predict
heavy states, a model with an extra gauge boson (Z0′) and
with a Kaluza-Klein (KK) excitation of the gluon (gKK). We
estimate the sensitive values of σ×Br of about 2 (4) fb
for Z0′ (gKK), with a corresponding mass reach of 13 (20)
TeV.},
Doi = {10.1103/PhysRevD.91.034014},
Key = {fds310307}
}
@article{fds346201,
Author = {Singh, M and Kotwal, A and Gupta, RM and Adhya, S and Chatterjee, K and Jayaram, J},
Title = {Sero-Epidemiological and Behavioural Survey of HIV, HBV and
HCV amongst Indian Armed Forces Trainees.},
Journal = {Medical journal, Armed Forces India},
Volume = {66},
Number = {1},
Pages = {50-54},
Year = {2010},
Month = {January},
url = {http://dx.doi.org/10.1016/s0377-1237(10)80093-0},
Abstract = {<h4>Background</h4>Information on the emerging epidemics of
Human immunodeficiency virus (HIV), Hepatitis B (HBV) and C
(HCV) viruses in younger age groups in India is scanty due
to paucity of representative, population based surveys and
varied estimation methodology. This study was done to assess
the point prevalence of HIV, HBV and HCV infections
alongwith the epidemiological factors associated with these
infections. Attitudes, beliefs and behaviour related to
sexual and injecting drug practices, with a view to assess
the need for introduction of screening program for the new
entrants of the armed forces was also studied.<h4>Methods</h4>A
multi-centric cross sectional serological and behavioural
survey was carried out amongst newly enrolled trainees of
the Armed Forces in 2004. The group was selected by
multistage random sampling giving equal representation to
all regions of India. Study subjects were interviewed using
a pretested, validated questionnaire and screened for HIV,
HBV and HCV infections by rapid tests. Standard confirmatory
tests were carried out for trainees testing positive.
Quality assurance measures were integral part of each
activity. A database was created in MS Access and SPSS ver
11.0.1 was used for analysis.<h4>Result</h4>Out of the
23,000 trainees included in the study, 22666 (98.55%) were
included in the analysis. The age, formal education and age
at first sexual intercourse of participants ranged from
16-25 years (median 20), 8-17 years (median 10) and 12-25
years, respectively. Partial knowledge about routes of
spread of HIV was highly prevalent but complete knowledge
was extremely low. Per thousand point prevalence of HIV, HBV
and HCV was 0.61 (95% CI, 0.34-10.3, poisson), 9.31
(8.1-10.65) and 4.44 (3.61-5.39), respectively. Clustering
of HIV (4.56 per 1000, 2.19-8.38) and HCV (30.54 per 1000,
23.67-38.78) and a higher number of HCV as compared to HBV
was found amongst trainees from northeast. A statistically
significant association was found between history of
injecting drug use (other than medical) and HCV
(p<0.05).<h4>Conclusion</h4>Self-exclusion for recruitment
as military trainees might have resulted in underestimation
of general population figures but results provide region
wise estimates unavailable till now. Concerted efforts are
required in the current HIV/AIDS program activities to bring
about knowledge and behaviour change amongst teenagers and
young adults.},
Doi = {10.1016/s0377-1237(10)80093-0},
Key = {fds346201}
}
@article{fds346180,
Author = {Kumar, S and Gupta, RM and Sen, S and Sarkar, RS and Philip, J and Kotwal,
A and Sumathi, SH},
Title = {Seroprevalence of human parvovirus B19 in healthy blood
donors.},
Journal = {Medical journal, Armed Forces India},
Volume = {69},
Number = {3},
Pages = {268-272},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.11.009},
Abstract = {<h4>Background</h4>Human parvovirus B19 is an emerging
transfusion transmitted infection. Although parvovirus B19
infection is connected with severe complications in some
recipients, donor screening is not yet mandatory. To reduce
the risk of contamination, plasma-pool screening and
exclusion of highly viraemic donations are recommended. In
this study the prevalence of parvovirus B19 in healthy blood
donors was detected by ELISA.<h4>Methods</h4>A total of 1633
samples were screened for IgM and IgG antibodies against
parvovirus B19 by ELISA. The initial 540 samples were
screened for both IgM and IgG class antibodies and remaining
1093 samples were screened for only IgM class antibodies by
ELISA.<h4>Results</h4>Net prevalence of IgM antibodies to
human parvovirus B19 in our study was 7.53% and prevalence
of IgG antibodies was 27.96%. Dual positivity (IgG and IgM)
was 2.40%.<h4>Conclusion</h4>The seroprevalence of human
parvovirus B19 among blood donor population in our study is
high, and poses an adverse transfusion risk especially in
high-risk group of patients who have no detectable
antibodies to B19. Studies with large sample size are needed
to validate these results.},
Doi = {10.1016/j.mjafi.2012.11.009},
Key = {fds346180}
}
@article{fds347531,
Author = {Kotwal, A and Cutrona, SL},
Title = {Serotonin Syndrome in the Setting of Lamotrigine,
Aripiprazole, and Cocaine Use.},
Journal = {Case reports in medicine},
Volume = {2015},
Pages = {769531},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1155/2015/769531},
Abstract = {Serotonin syndrome is a potentially life-threatening
condition associated with increased serotonergic activity in
the central nervous system. It is classically associated
with the simultaneous administration of two serotonergic
agents, but it can occur after initiation of a single
serotonergic drug or increasing the dose of a serotonergic
drug in individuals who are particularly sensitive to
serotonin. We describe a case of serotonin syndrome that
occurred after ingestion of higher than prescribed doses of
lamotrigine and aripiprazole, in addition to cocaine abuse.
The diagnosis was established based on Hunter toxicity
criteria and severity was classified as mild. The features
of this syndrome resolved shortly after discontinuation of
the offending agents. Serotonin syndrome is characterized by
mental status changes, autonomic hyperactivity, and
neuromuscular abnormalities along a spectrum ranging from
mild to severe. Serotonin syndrome in our patient was most
likely caused by the pharmacokinetic and pharmacodynamic
interactions between lamotrigine, aripiprazole, and cocaine
leading to increased CNS serotonergic activity.},
Doi = {10.1155/2015/769531},
Key = {fds347531}
}
@booklet{Adams95,
Author = {Adams, MR and Aïd, S and Anthony, PL and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Breidung, H and Busza, W and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dhawan, SK and Dietrich, FS and Dougherty,
W and Dreyer, T and Eckardt, V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen,
KA and Guo, RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Hughes, VW and Jackson, HE and Jaffe, DE and Jancso, G and Jansen, DM and Jin, Z and Kaufman, S and Kennedy, RD and Kinney, ER and Kirk, T and Kobrak, HGE and Kotwal, AV and Kunori, S and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Magill, S and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin, JG and Nickerson, RB and Novak, J and O'Day, S and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Ramberg, EJ and Röser, A and Ryan, JJ and Salgado, CW and Salvarani, A and Schellman, H and Schmitt, M and Schmitz, N and Schüler, KP and Siegert,
G and Skuja, A and Snow, GA and Söldner-Rembold, S and Spentzouris, P and Stier, HE and Stopa, P and Swanson, RA and Venkataramania, H and Wilhelm, M and Wilson, R and Wittek, W and Wolbers, SA and Zghiche, A and Zhao, T},
Title = {Shadowing in inelastic scattering of muons on carbon,
calcium and lead at low xBj},
Journal = {Zeitschrift für Physik C Particles and Fields},
Volume = {67},
Number = {3},
Pages = {403-410},
Publisher = {Springer Nature},
Year = {1995},
Month = {September},
url = {http://dx.doi.org/10.1007/BF01624583},
Abstract = {Nuclear shadowing is observed in the per-nucleon cross
sections of positive muons on carbon, calcium and lead as
compared to deuterium. The data were taken by Fermilab
experiment E665 using inelastically scattered muons of mean
incident momentum 470 GeV/c. Cross-section ratios are
presented in the kinematic region 0.0001<xBj<0.56 and
0.1<Q2<80 GeV2. The data are consistent with no significant
ν or Q2 dependence at fixed xBj. As xBj decreases, the size
of the shadowing effect, as well as its A dependence, are
found to approach the corresponding measurements in
photoproduction. © 1995 Springer-Verlag.},
Doi = {10.1007/BF01624583},
Key = {Adams95}
}
@article{fds307584,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Signature-based search for delayed photons in exclusive
photon plus missing transverse energy events from pp̄
collisions with √s=1.96 TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {3},
Pages = {031103},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.88.031103},
Abstract = {We present the first signature-based search for delayed
photons using an exclusive photon plus missing transverse
energy final state. Events are reconstructed in a data
sample from the CDF II detector corresponding to 6.3 fb-1 of
integrated luminosity from √s=1.96 TeV proton-antiproton
collisions. Candidate events are selected if they contain a
photon with an arrival time in the detector larger than
expected from a promptly produced photon. The mean number of
events from standard model sources predicted by the
data-driven background model based on the photon timing
distribution is 286±24. A total of 322 events are observed.
A p value of 12% is obtained, showing consistency of the
data with standard model predictions. © 2013 American
Physical Society.},
Doi = {10.1103/PhysRevD.88.031103},
Key = {fds307584}
}
@article{fds310297,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V},
Title = {Simultaneous measurements of the tt¯, W+W-, and Z/γ∗
→ττ production cross-sections in pp collisions at √s
=7 TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2015},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.91.052005},
Abstract = {Simultaneous measurements of the tt¯, W+W-, and
Z/γ∗→ττ production cross-sections using an integrated
luminosity of 4.6 fb-1 of pp collisions at √s=7 TeV
collected by the ATLAS detector at the LHC are presented.
Events are selected with two high transverse momentum
leptons consisting of an oppositely charged electron and
muon pair. The three processes are separated using the
distributions of the missing transverse momentum of events
with zero and greater than zero jet multiplicities.
Measurements of the fiducial cross-section are presented
along with results that quantify for the first time the
underlying correlations in the predicted and measured
cross-sections due to proton parton distribution functions.
These results indicate that the correlated
next-to-leading-order predictions for tt¯ and
Z/γ∗→ττ underestimate the data, while those at
next-to-next-to-leading-order generally describe the data
well. The full cross-sections are measured to be
σ(tt¯)=181.2±2.8-9.5+9.7±3.3±3.3 pb,
σ(W+W-)=53.3±2.7-8.0+7.3±1.0±0.5 pb, and
σ(Z/γ∗→ττ)=1174±24-87+72±21±9 pb, where the cited
uncertainties are due to statistics, systematic effects,
luminosity and the LHC beam energy measurement,
respectively. The W+W- measurement includes the small
contribution from Higgs boson decays, H→W+W-.},
Doi = {10.1103/PhysRevD.91.052005},
Key = {fds310297}
}
@article{fds307620,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Zeid, OSA and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allbrooke, BMM and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Gonzalez, BA and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Bella, LA and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik,
M and Armbruster, AJ and Arnaez, O},
Title = {Single hadron response measurement and calorimeter jet
energy scale uncertainty with the ATLAS detector at the
LHC},
Journal = {European Physical Journal C},
Volume = {73},
Number = {3},
Publisher = {Springer Nature},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-013-2305-1},
Abstract = {The uncertainty on the calorimeter energy response to jets
of particles is derived for the ATLAS experiment at the
Large Hadron Collider (LHC). First, the calorimeter response
to single isolated charged hadrons is measured and compared
to the Monte Carlo simulation using proton-proton collisions
at centre-of-mass energies of √s = 900 GeV and 7 TeV
collected during 2009 and 2010. Then, using the decay of
K<inf>s</inf> and Λ particles, the calorimeter response to
specific types of particles (positively and negatively
charged pions, protons, and anti-protons) is measured and
compared to the Monte Carlo predictions. Finally, the jet
energy scale uncertainty is determined by propagating the
response uncertainty for single charged and neutral
particles to jets. The response uncertainty is 2–5 % for
central isolated hadrons and 1–3 % for the final
calorimeter jet energy scale.},
Doi = {10.1140/epjc/s10052-013-2305-1},
Key = {fds307620}
}
@article{fds322004,
Author = {Kotwal, AV and Ramsey-Musolf, MJ and No, JM and Winslow,
P},
Title = {Singlet-catalyzed electroweak phase transitions in the 100
TeV frontier SINGLET-CATALYZED ELECTROWEAK PHASE ... KOTWAL
et al.},
Journal = {Physical Review D},
Volume = {94},
Number = {3},
Publisher = {American Physical Society (APS)},
Year = {2016},
Month = {August},
url = {http://dx.doi.org/10.1103/PhysRevD.94.035022},
Abstract = {We study the prospects for probing a gauge singlet
scalar-driven strong first-order electroweak phase
transition with a future proton-proton collider in the 100
TeV range. Singlet-Higgs mixing enables resonantly enhanced
di-Higgs production, potentially aiding discovery prospects.
We perform Monte Carlo scans of the parameter space to
identify regions associated with a strong first-order
electroweak phase transition, analyze the corresponding
di-Higgs signal, and select a set of benchmark points that
span the range of di-Higgs signal strengths. For the bbγγ
and 4τ final states, we investigate discovery prospects for
each benchmark point for the high-luminosity phase of the
Large Hadron Collider and for a future pp collider with
s=50, 100, or 200 TeV. We find that any of these future
collider scenarios could significantly extend the reach
beyond that of the high-luminosity LHC, and that with s=100
TeV (200 TeV) and 30 ab-1, the full region of parameter
space favorable to strong first-order electroweak phase
transitions is almost fully (fully) discoverable.},
Doi = {10.1103/PhysRevD.94.035022},
Key = {fds322004}
}
@article{fds308211,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Balamurali, V and Baldin, B and Banerjee,
S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding,
F and Boswell, C and Brandt, A and Breedon, R and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey,
D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang,
SM and Chekulaev, SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark,
AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Cretsinger,
C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del Signore and K and Demarteau, M and Denisov, D and Denisov, SP and Diehl, HT and Diesburg, M and Di Loreto and G and Draper,
P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G},
Title = {Small angle J/ψ production in pp¯ collisions at
√s=1.8TeV},
Journal = {Physical Review Letters},
Volume = {82},
Number = {1},
Pages = {35-40},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.82.35},
Abstract = {This paper presents the first measurement of inclusive J/ψ
production cross section in the forward pseudorapidity
region 2.5≤|ηJ/ψ|≤3.7 in pp¯ collisions at √S=1.8
TeV. The results are based on 9.8 pb−1 of data collected
using the D0 detector at the Fermilab Tevatron Collider. The
inclusive J/ψ cross section for transverse momenta between
1 and 16 GeV/c is compared with theoretical models of
charmonium production. © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.82.35},
Key = {fds308211}
}
@article{fds308199,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler,
JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and di Loreto, G and Draper, P and Ducros, Y and Dudko,
LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Fatyga,
MK and Feher, S and Fein, D and Ferbel, T},
Title = {Small-angle muon and bottom-quark production in pp̄
collisions at √s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {84},
Number = {24},
Pages = {5478-5483},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevLett.84.5478},
Abstract = {The inclusive muon cross section, and the cross section for
mouns originating from b quark decay, in the forward
rapidity region of 2.4 < | ymu | < 3.2 were measured in this
study. It was found that next-to-leading order QCD
calculations underestimate b quark production by a factor of
4 in this region.},
Doi = {10.1103/PhysRevLett.84.5478},
Key = {fds308199}
}
@article{fds362574,
Author = {Agashe, K and Erbacher, R and Gerber, CE and Melnikov, K and Schwienhorst, R and Mitov, A and Vos, M and Wimpenny, S and Adelman, J and Baumgart, M and Garcia-Bellido, A and Loginov, A and Jung, A and Schulze, M and Shelton, J and Craig, N and Velasco, M and Golling, T and Hubisz, J and Ivanov, A and Perelstein, M and Chekanov, S and Dolen, J and Pilot, J and Pöschl, R and Tweedie, B and Alioli, S and Alvarez-Gonzalez, B and Amidei, D and Andeen, T and Arce, A and Auerbach, B and Avetisyan, A and Backovic, M and Bai, Y and Begel, M and Berge, S and Bernard, C and Bernius, C and Bhattacharya, S and Black, K and Blondel, A and Bloom, K and Bose, T and Boudreau, J and Brau, J and Broggio, A and Brooijmans, G and Brost, E and Calkins, R and Chakraborty, D and Childress, T and Choudalakis, G and Coco, V and Conway, JS and Degrande, C and Delannoy, A and Deliot, F and Dell'Asta,
L and Drueke, E and Dutta, B and Effron, A and Ellis, K and Erdmann, J and Evans, J and Feng, C and Feng, E and Ferroglia, A and Finelli, K and Flanagan, W and Fleck, I and Freitas, A and Garberson, F and Suarez, RG and Graesser, ML and Graf, N and Greenwood, Z and George, J and Group, C and Gurrola, A and Hammad, G and Han, T and Han, Z and Heintz, U and Hoeche, S and Horiguchi, T and Iashvili, I and Ismail, A and Jain, S and Janot, P and Johns, W and Joshi, J and Juste, A and Kamon, T and Kao, C and Kats, Y and Katz, A and Kaur, M and Kehoe, R and Keung, W and Khalil, S and Khanov, A and Kharchilava, A and Kidonakis, N and Kilic, C and Kolev, N and Kotwal, A and Kraus, J and Krohn, D and Kruse, M and Kumar, A and Lee, S and Luiggi, E and Mantry, S and Melo, A and Miller, D and Moortgat-Pick, G and Narain, M and Odell, N and Oksuzian, Y and Oreglia, M and Penin, A and Peters, Y and Pollard, C and Poss, S and Rappoccio, HBPS and Redford, S and Reece, M and Rizatdinova, F and Roloff, P and Ruiz, R and Saleem, M and Schoenrock,
B and Schwanenberger, C and Schwarz, T and Seidel, K and Shabalina, E and Sheldon, P and Simon, F and Sinha, K and Skands, P and Skubik, P and Sterman, G and Stolarski, D and Strube, J and Stupak, J and Su, S and Tesar, M and Thomas, S and Thompson, E and Tipton, P and Varnes, E and Vignaroli, N and Virzi, J and Vogel, M and Walker, D and Wang, K and Webber, B and Wells, JD and Westhoff, S and Whiteson, D and Williams, M and Wu, S and Yang, U and Yokoya, H and Yoo, H and Zhang, H and Zhou, N and Zhu,
H and Zupan, J},
Title = {Snowmass 2013 Top quark working group report},
Year = {2013},
Month = {November},
Abstract = {This report summarizes the work of the Energy Frontier Top
Quark working group of the 2013 Community Summer Study
(Snowmass).},
Key = {fds362574}
}
@article{fds362578,
Author = {Anderson, J and Avetisyan, A and Brock, R and Chekanov, S and Cohen, T and Dhingra, N and Dolen, J and Hirschauer, J and Howe, K and Kotwal, A and LeCompte, T and Malik, S and Mcbride, P and Mishra, K and Narain, M and Olsen, J and Padhi, S and Peskin, ME and III, JS and Wacker,
JG},
Title = {Snowmass Energy Frontier Simulations},
Year = {2013},
Month = {September},
Abstract = {This document describes the simulation framework used in the
Snowmass Energy Frontier studies for future Hadron
Colliders. An overview of event generation with {\sc
Madgraph}5 along with parton shower and hadronization with
{\sc Pythia}6 is followed by a detailed description of
pile-up and detector simulation with {\sc Delphes}3. Details
of event generation are included in a companion paper cited
within this paper. The input parametrization is chosen to
reflect the best object performance expected from the future
ATLAS and CMS experiments; this is referred to as the
"Combined Snowmass Detector". We perform simulations of $pp$
interactions at center-of-mass energies $\sqrt{s}=$ 14, 33,
and 100 TeV with 0, 50, and 140 additional $pp$ pile-up
interactions. The object performance with multi-TeV $pp$
collisions are studied for the first time using large
pile-up interactions.},
Key = {fds362578}
}
@article{fds308207,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buescher,
V and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum,
Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev,
SV and Chen, W and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis,
K and De, K and del Signore, K and Demarteau, M and Denisov, D and Denisov,
SP and Diehl, HT and Diesburg, M and di Loreto, G and Draper, P and Ducros,
Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison,
J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland,
T and Feher, S and Fein, D and Ferbel, T},
Title = {Spin correlation in tt̄ production from pp̄ collisions at
√s = 1.8 TeV},
Journal = {Physical Review Letters},
Volume = {85},
Number = {2},
Pages = {256-261},
Publisher = {American Physical Society (APS)},
Year = {2000},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevLett.85.256},
Abstract = {An analytical study was carried out to account for spin
correlation effects in the production of tt̄ pairs in pp̄
collisions at √s=1.8 TeV. It was found that κ > -0.25 at
the 68% confidence level.},
Doi = {10.1103/PhysRevLett.85.256},
Key = {fds308207}
}
@article{fds316845,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adye, T and Aefsky, S and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmad, A and Ahmadov, F and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso,
A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi,
MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami,
A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Standalone vertex finding in the ATLAS muon
spectrometer},
Journal = {Journal of Instrumentation},
Volume = {9},
Number = {2},
Pages = {P02001-P02001},
Publisher = {IOP Publishing},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/9/02/P02001},
Abstract = {A dedicated reconstruction algorithm to find decay vertices
in the ATLAS muon spectrometer is presented. The algorithm
searches the region just upstream of or inside the muon
spectrometer volume for multi-particle vertices that
originate from the decay of particles with long decay paths.
The performance of the algorithm is evaluated using both a
sample of simulated Higgs boson events, in which the Higgs
boson decays to long-lived neutral particles that in turn
decay to bb final states, and pp collision data at √s = 7
TeV collected with the ATLAS detector at the LHC during
2011.},
Doi = {10.1088/1748-0221/9/02/P02001},
Key = {fds316845}
}
@article{fds308158,
Author = {Kotwal, A},
Title = {Status and plans of the tevatron electroweak working
group},
Journal = {AIP Conference Proceedings},
Volume = {753},
Pages = {149-157},
Publisher = {AIP},
Year = {2005},
Month = {March},
url = {http://dx.doi.org/10.1063/1.1896697},
Abstract = {The Tevatron Electroweak Working group was created in
September, 2003 at Fermilab to consolidate electroweak
physics results for precision Standard Model tests. It is
the first combined analysis group at Fermilab to publish in
a refereed journal. The group currently has 49 subscribers.
Three subgroups are dedicated to studies of W and Z boson
properties, top quark properties, and Higgs physics
respectively. The group has produced combined results from
the CDF and DØ experiments on the Run 1 W boson mass and
width, the Run 1 top quark mass, and the Run 2 measurement
of the ratio of W and Z boson cross sections. New results
are anticipated as Run 2 analyses mature. The group also
organizes joint workshops for theorists and
experimentalists. © 2005 American Institute of
Physics.},
Doi = {10.1063/1.1896697},
Key = {fds308158}
}
@article{fds346203,
Author = {Roshan, A and Kotwal, A and Riaz, M and Stanley, PRW},
Title = {Sternal wound dehiscence complicated by macromastia: report
of two cases with discussion of literature.},
Journal = {Journal of plastic, reconstructive & aesthetic surgery :
JPRAS},
Volume = {62},
Number = {10},
Pages = {e362-e364},
Year = {2009},
Month = {October},
url = {http://dx.doi.org/10.1016/j.bjps.2008.02.019},
Abstract = {Sternal wound dehiscence complicated by macromastia can be
difficult to treat by standard musculocutaneous flaps alone.
We present our experience with two cases of sternal wound
dehiscence complicated by macromastia, and their subsequent
healing with a combination of reduction mammoplasty and
local musculocutaneous flaps. Reduction mammoplasty is a
useful adjunctive procedure in patients with macromastia
complicating sternal wound dehiscence.},
Doi = {10.1016/j.bjps.2008.02.019},
Key = {fds346203}
}
@article{fds346197,
Author = {Sinha, A and Kushwaha, AS and Kotwal, A and Sanghi, S and Verma,
AK},
Title = {Stigma in leprosy: miles to go!},
Journal = {Indian journal of leprosy},
Volume = {82},
Number = {3},
Pages = {137-145},
Year = {2010},
Month = {July},
Abstract = {No disease has been more closely associated with stigma than
leprosy such that it has become a metaphor for stigma.
Stigma has been difficult to measure and little research has
been done on this issue. Stigma reduction has not been an
important component of anti-leprosy program. The study was
undertaken to measure the stigma associated with leprosy by
using P scale which is used for assessing participation
restriction of those affected by the disease. This
comparative questionnaire based study was carried out in two
sets of patients. Two groups of 30 patients each were
studied. First group belonged to a Government run
Leprosarium and group two from a tertiary care skin and
leprosy centre. The study used the Participation (P) scale
and data was collected by interviewing the patients.
Participation restriction was defined as any score equal to
and more than 13. Participation restriction was observed in
27 (90%) cases of group 1while participation restriction was
present in only 7 (23.3%) subjects of group 2. It was
observed that mean score of participation restriction in
group 1 was quite high at 31.9 while it was only 8.3 for
group 2. The participation restriction was directly related
to the duration of disease and the grade of disability.
Longer the duration of disease, greater was the likelihood
of restriction. The participation restriction was found to
be negatively correlated with the education. Recommendation
about prevention of disability would require program about
early diagnosis of nerve damage and subsequent action at the
patient-family-community level and health care
providers.},
Key = {fds346197}
}
@article{fds346217,
Author = {Seth, R and Kotwal, A and Ganguly, KK},
Title = {Street and working children of Delhi, India, misusing
toluene: an ethnographic exploration.},
Journal = {Substance use & misuse},
Volume = {40},
Number = {11},
Pages = {1659-1679},
Year = {2005},
Month = {January},
url = {http://dx.doi.org/10.1080/10826080500222792},
Abstract = {Our qualitative study explored: the perceptions of street
children indulging in whitener fluid misuse; the social,
economic, and cultural determinants of use; and users' views
regarding effective preventive and control strategies.
Forty-five in-depth interviews and three focus group
discussions were conducted between March and December 2003.
A purposive sample of those working children who were using
toluene was selected by Snowball sampling. The paper
discusses the: determinants of initiation and continued use;
drug user social networks; psycho emotional deprivation and
frustrations of these children; socio-cultural aspects like
work driven need; others' attitudinal response towards them
and their work; parental support or the lack of it; and
strategies for prevention of this misuse.},
Doi = {10.1080/10826080500222792},
Key = {fds346217}
}
@article{fds372604,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam, L and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Amrouche, CS and Ananiev, V and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Asimakopoulou, EM and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson,
M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol, AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends,
KN and Barillari, T and Barisits, M-S and Barkeloo, J and Barklow, T and Barnett, RM and Baron, P and Baron Moreno and DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira,
MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos,
P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat,
A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley,
JR and Batool, B and Battaglia, M and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle,
P and Beck, HP and Becker, K and Becot, C and Beddall, AJ and Bednyakov,
VA and Bee, CP and Beemster, LJ and Beermann, TA and Begalli, M and Begel,
M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer,
JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos, P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun, D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi,
G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram, IA and Bessidskaia Bylund and O and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya,
DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel,
O and Bielski, R and Biglietti, M and Billoud, TRV and Bindi, M and Bingul,
A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird,
GA and Birman, M and Bisanz, T and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal,
J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Breaden Madden and WD and Brendlinger, K and Brener, R and Brenner,
L and Brenner, R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock, I and Brooijmans, G and Brooks, WK and Brost, E and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlson, BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter, JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo
Garcia, L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi,
E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri,
A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WS and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton, DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen,
SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli,
G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu, YH and Chizhov,
MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clavijo Columbie and JM and Clawson, SE and Clement, C},
Title = {Strong Constraints on Jet Quenching in Centrality-Dependent
p+Pb Collisions at 5.02 TeV from ATLAS.},
Journal = {Physical review letters},
Volume = {131},
Number = {7},
Pages = {072301},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.131.072301},
Abstract = {Jet quenching is the process of color-charged partons losing
energy via interactions with quark-gluon plasma droplets
created in heavy-ion collisions. The collective expansion of
such droplets is well described by viscous hydrodynamics.
Similar evidence of collectivity is consistently observed in
smaller collision systems, including pp and p+Pb collisions.
In contrast, while jet quenching is observed in Pb+Pb
collisions, no evidence has been found in these small
systems to date, raising fundamental questions about the
nature of the system created in these collisions. The ATLAS
experiment at the Large Hadron Collider has measured the
yield of charged hadrons correlated with reconstructed jets
in 0.36 nb^{-1} of p+Pb and 3.6 pb^{-1} of pp
collisions at 5.02 TeV. The yields of charged hadrons with
p_{T}^{ch}>0.5 GeV near and opposite in azimuth to jets
with p_{T}^{jet}>30 or 60 GeV, and the ratios of these
yields between p+Pb and pp collisions, I_{pPb}, are
reported. The collision centrality of p+Pb events is
categorized by the energy deposited by forward neutrons from
the struck nucleus. The I_{pPb} values are consistent with
unity within a few percent for hadrons with
p_{T}^{ch}>4 GeV at all centralities. These data
provide new, strong constraints that preclude almost any
parton energy loss in central p+Pb collisions.},
Doi = {10.1103/physrevlett.131.072301},
Key = {fds372604}
}
@booklet{Abachi97,
Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard, J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G and Fisk, HE},
Title = {Studies of gauge boson pair production and trilinear
couplings},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {56},
Number = {11},
Pages = {6742-6778},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.56.6742},
Abstract = {The gauge boson pair production processes [Formula
presented], [Formula presented], [Formula presented], and
[Formula presented] were studied using [Formula presented]
collisions corresponding to an integrated luminosity of
approximately [Formula presented] at a center-of-mass energy
of [Formula presented] TeV. Analysis of [Formula presented]
production with subsequent [Formula presented] boson decay
to [Formula presented] [Formula presented] is reported,
including a fit to the [Formula presented] spectrum of the
photons which leads to limits on anomalous [Formula
presented] couplings. A search for [Formula presented]
production with subsequent decay to [Formula presented]
[Formula presented] is presented, leading to an upper limit
on the [Formula presented] production cross section and
limits on anomalous [Formula presented] and [Formula
presented] couplings. A search for high [Formula presented]
[Formula presented] bosons in [Formula presented] and
[Formula presented] production is described, where one
[Formula presented] boson decays to an electron and a
neutrino and the second [Formula presented] boson or the
[Formula presented] boson decays to two jets. A maximum
likelihood fit to the [Formula presented] spectrum of
[Formula presented] bosons resulted in limits on anomalous
[Formula presented] and [Formula presented] couplings. A
combined fit to the three data sets which provided the
tightest limits on anomalous [Formula presented] and
[Formula presented] couplings is also described. Limits on
anomalous [Formula presented] and [Formula presented]
couplings are presented from an analysis of the photon
[Formula presented] spectrum in [Formula presented] events
in the decay channels [Formula presented] of the [Formula
presented] boson. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevD.56.6742},
Key = {Abachi97}
}
@article{fds345677,
Author = {Yeh, CH and Chekanov, SV and Kotwal, AV and Proudfoot, J and Sen, S and Tran, NV and Yu, SS},
Title = {Studies of granularity of a hadronic calorimeter for
tens-of-TeV jets at a 100 TeV pp collider},
Journal = {Journal of Instrumentation},
Volume = {14},
Number = {5},
Year = {2019},
Month = {May},
url = {http://dx.doi.org/10.1088/1748-0221/14/05/P05008},
Abstract = {Jet substructure variables for hadronic jets with transverse
momenta in the range from 2.5 TeV to 20 TeV were studied
using several designs for the spatial size of calorimeter
cells. The studies used the full Geant4 simulation of
calorimeter response combined with realistic reconstruction
of calorimeter clusters. In most cases, the results indicate
that the performance of jet-substructure reconstruction
improves with reducing cell size of a hadronic calorimeter
from Δ η × Δ φ = 0.087×0.087, which are similar to the
cell sizes of the calorimeters of LHC experiments, by a
factor of four, to 0.022×0.022.},
Doi = {10.1088/1748-0221/14/05/P05008},
Key = {fds345677}
}
@article{fds310306,
Author = {Aaltonen, T and Alon, R and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Duchovni, E and Ebina, K and Edgar, R and Elagin,
A},
Title = {Studies of high-transverse momentum jet substructure and top
quarks produced in 1.96 TeV proton-antiproton
collisions},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {91},
Number = {3},
Year = {2015},
Month = {February},
url = {http://dx.doi.org/10.1103/PhysRevD.91.032006},
Abstract = {Results of a study of the substructure of the highest
transverse momentum (pT) jets observed by the CDF
Collaboration are presented. Events containing at least one
jet with pT>400GeV/c in a sample corresponding to an
integrated luminosity of 5.95fb-1, collected in 1.96 TeV
proton-antiproton collisions at the Fermilab Tevatron
collider, are selected. A study of the jet mass, angularity,
and planar-flow distributions is presented, and the
measurements are compared with predictions of perturbative
quantum chromodynamics. A search for boosted top-quark
production is also described, leading to a 95% confidence
level upper limit of 38 fb on the production cross section
of top quarks with pT>400GeV/c.},
Doi = {10.1103/PhysRevD.91.032006},
Key = {fds310306}
}
@article{fds374252,
Author = {Aad, G and Abbott, B and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akolkar, NN and Khoury, KA and Alberghi, GL and Albert,
J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Alkakhi,
W and Allaire, C and Allbrooke, BMM and Allendes Flores and CA and Allport,
PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alviggi, MG and Aly, M and Amaral Coutinho,
Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo,
MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz,
V and Arcangeletti, C and Arce, ATH},
Title = {Studies of the muon momentum calibration and performance of
the ATLAS detector with pp collisions at √s=13
TeV},
Journal = {European Physical Journal C},
Volume = {83},
Number = {8},
Publisher = {Springer Science and Business Media LLC},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1140/epjc/s10052-023-11584-x},
Abstract = {This paper presents the muon momentum calibration and
performance studies for the ATLAS detector based on the pp
collisions data sample produced at s = 13 TeV at the LHC
during Run 2 and corresponding to an integrated luminosity
of 139 fb - 1 . An innovative approach is used to correct
for potential charge-dependent momentum biases related to
the knowledge of the detector geometry, using the Z→
μ+μ- resonance. The muon momentum scale and resolution are
measured using samples of J/ ψ→ μ+μ- and Z→ μ+μ-
events. A calibration procedure is defined and applied to
simulated data to match the performance measured in real
data. The calibration is validated using an independent
sample of Υ → μ+μ- events. At the Z (J/ ψ) peak, the
momentum scale is measured with an uncertainty at the 0.05%
(0.1%) level, and the resolution is measured with an
uncertainty at the 1.5% (2%) level. The charge-dependent
bias is removed with a dedicated in situ correction for
momenta up to 450 GeV with a precision better than 0.03 TeV
- 1 .},
Doi = {10.1140/epjc/s10052-023-11584-x},
Key = {fds374252}
}
@article{fds362577,
Author = {Degrande, C and Holzbauer, JL and Hsu, S-C and Kotwal, AV and Li, S and Marx, M and Mattelaer, O and Metcalfe, J and Pleier, M-A and Pollard, C and Rominsky, M and Wackeroth, D},
Title = {Studies of Vector Boson Scattering And Triboson Production
with DELPHES Parametrized Fast Simulation for Snowmass
2013},
Year = {2013},
Month = {September},
Abstract = {Multiboson production provides a unique way to probe
Electroweak Symmetry Breaking (EWSB) and physics beyond the
Standard Model (SM). With the discovery of the Higgs boson,
the default model is that EWSB occurs according to the Higgs
mechanism. Deviations from the SM in Higgs and gauge boson
properties due to new physics at a higher energy scale can
be parameterized by higher-dimension operators in an
Effective Field Theory (EFT). We present sensitivity studies
for dimension-6 and dimension-8 operators in an EFT by
looking for anomalous vector boson scattering and triboson
production, at proton-proton colliders with center-of-mass
energies of 14 TeV, 33 TeV and 100 TeV, respectively.},
Key = {fds362577}
}
@article{fds212568,
Author = {A.V. Kotwal and ATLAS Collaboration},
Title = {Studies of Vector Boson Scattering with an Upgraded ATLAS
Detector at a High-Luminosity LHC},
Journal = {ATLAS-PHYS-PUB-2012-005},
Year = {2012},
Month = {November},
Key = {fds212568}
}
@article{fds308219,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom, P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Breedon,
R and Briskin, G and Brock, R and Bross, A and Buchholz, D and Burtovoi,
VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chekulaev, SV and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung,
M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Cooper, WE and Coppage, D and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros, Y and Dudko,
LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira,
VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin,
OV and Evans, H and Evdokimov, VN and Fahland, T and Fatyga, MK and Feher,
S and Fein, D and Ferbel, T and Fisk, HE and Fisyak,
Y},
Title = {Studies of WW and WZ production and limits on anomalous WWγ
and WWZ couplings},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {60},
Number = {7},
Pages = {1-14},
Publisher = {American Physical Society (APS)},
Year = {1999},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.60.072002},
Abstract = {Evidence of anomalous (Formula presented) and (Formula
presented) production was sought in (Formula presented)
collisions at a center-of-mass energy of (Formula presented)
The final states (Formula presented) jet (Formula presented)
(Formula presented) and (Formula presented) were studied
using a data sample corresponding to an integrated
luminosity of approximately (Formula presented) No evidence
of anomalous diboson production was found. Limits were set
on anomalous (Formula presented) and (Formula presented)
couplings and were combined with our previous results. The
combined 95% confidence level anomalous coupling limits for
(Formula presented) are (Formula presented) (Formula
presented) and (Formula presented) (Formula presented)
assuming the (Formula presented) couplings are equal to the
(Formula presented) couplings. © 1999 The American Physical
Society.},
Doi = {10.1103/PhysRevD.60.072002},
Key = {fds308219}
}
@article{fds356748,
Author = {The ATLAS collaboration, and Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and AbouZeid,
OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman,
J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin,
T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Alconada Verzini,
MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari,
N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo
Ferraz, V and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Studies of Zγ production in association with a high-mass
dijet system in pp collisions at √s=8 TeV with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {7},
Year = {2017},
Month = {July},
url = {http://dx.doi.org/10.1007/JHEP07(2017)107},
Abstract = {The production of a Z boson and a photon in association with
a high-mass dijet system is studied using 20.2 fb−1 of
proton-proton collision data at a centre-of-mass energy of
s=8 TeV recorded with the ATLAS detector in 2012 at the
Large Hadron Collider. Final states with a photon and a Z
boson decaying into a pair of either electrons, muons, or
neutrinos are analysed. Electroweak and total pp → Zγjj
cross-sections are extracted in two fiducial regions with
different sensitivities to electroweak production processes.
Quartic couplings of vector bosons are studied in regions of
phase space with an enhanced contribution from pure
electroweak production, sensitive to vector-boson scattering
processes VV → Zγ. No deviations from Standard Model
predictions are observed and constraints are placed on
anomalous couplings parameterized by higher-dimensional
operators using effective field theory.[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP07(2017)107},
Key = {fds356748}
}
@article{fds317299,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto,
G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada
Verzini, MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Study of (W/Z)H production and Higgs boson couplings using
H→ W W∗ decays with the ATLAS
detector},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {8},
Publisher = {Springer Nature},
Year = {2015},
Month = {August},
url = {http://dx.doi.org/10.1007/JHEP08(2015)137},
Abstract = {Abstract: A search for Higgs boson production in association
with a W or Z boson, in the H→ W W∗ decay channel, is
performed with a data sample collected with the ATLAS
detector at the LHC in proton-proton collisions at
centre-of-mass energies √s=7$$ \sqrt{s}=7 $$ TeV and 8
TeV, corresponding to integrated luminosities of 4.5 fb−1
and 20.3 fb−1, respectively. The WH production mode is
studied in two-lepton and three-lepton final states, while
two- lepton and four-lepton final states are used to search
for the ZH production mode. The observed significance, for
the combined W H and ZH production, is 2.5 standard
deviations while a significance of 0.9 standard deviations
is expected in the Standard Model Higgs boson hypothesis.
The ratio of the combined W H and ZH signal yield to the
Standard Model expectation, μV H , is found to be μV H =
3.0− 1.1+ 1.3(stat.)− 0.7+ 1.0(sys.) for the Higgs boson
mass of 125.36 GeV. The W H and ZH production modes are also
combined with the gluon fusion and vector boson fusion
production modes studied in the H → W W∗ → ℓνℓν
decay channel, resulting in an overall observed significance
of 6.5 standard deviations and μggF + VBF + VH = 1. 16−
0.15+ 0.16(stat.)− 0.15+ 0.18(sys.). The results are
interpreted in terms of scaling factors of the Higgs boson
couplings to vector bosons (κV ) and fermions (κF ); the
combined results are: |κV| = 1.06− 0.10+ 0.10, |κF| = 0.
85− 0.20+ 0.26.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP08(2015)137},
Key = {fds317299}
}
@article{fds346186,
Author = {Reddy, D and Kushwaha, AS and Kotwal, A and Basannar, DR and Mahen,
A},
Title = {Study of blood pressure profile of school children 6-15
years in a rural setting of Maharashtra.},
Journal = {Medical journal, Armed Forces India},
Volume = {68},
Number = {3},
Pages = {222-225},
Year = {2012},
Month = {July},
url = {http://dx.doi.org/10.1016/j.mjafi.2012.03.004},
Abstract = {<h4>Background</h4>High blood pressure in childhood is a
major risk factor for heart disease and stroke in adulthood.
There is enough evidence to suggest that the roots of
essential hypertension in adults extend into childhood.
There is a paucity of literature on the blood pressure
measurements amongst children. This study was done to study
blood pressure profile of school children in rural area of
Maharashtra.<h4>Aim & objectives</h4>This cross sectional
study was carried out to determine the prevalence of
hypertension in children 6-15 years and to study the
association between selected variables and blood
pressure.<h4>Material & methods</h4>This study was done
using a predesigned questionnaire and making measurements of
height, BMI and Blood pressure using standardized physical
instruments following standard guidelines. The data was
collected and analyzed using appropriate statistical
tests.<h4>Results</h4>The prevalence of hypertension in the
study was found to be 4.4% with 3.5% in females and 5.1% in
males.<h4>Conclusion</h4>In the study, hypertension in
students was found to be significantly associated with
higher BMI and with family history of hypertension. Age,
height and BMI were found to correlate positively with Blood
pressure levels in this study.},
Doi = {10.1016/j.mjafi.2012.03.004},
Key = {fds346186}
}
@article{fds327865,
Author = {Yu, SS and Chekanov, S and Gray, L and Kotwal, A and Sen, S and Tran,
NV},
Title = {Study of boosted W-jets and Higgs-jets with the SiFCC
detector},
Journal = {Proceedings of Science},
Volume = {Part F128556},
Year = {2016},
Month = {January},
Abstract = {We study the detector performance in the reconstruction of
hadronically-decaying W bosons and Higgs bosons at very high
energy proton colliders using a full Geant4 simulation of
the SiFCC detector. The W and Higgs bosons carry transverse
momentum in the multi-TeV range, which results in collimated
decay products that are reconstructed as a single jet. We
present a measurement of the energy response and resolution
of boosted W-jets and Higgs-jets and show the separation of
two sub-jets within the boosted boson jet.},
Key = {fds327865}
}
@article{fds362576,
Author = {Baak, M and Blondel, A and Bodek, A and Caputo, R and Corbett, T and Degrande, C and Eboli, O and Erler, J and Feigl, B and Freitas, A and Fraile, JG and Gonzalez-Garcia, MC and Haller, J and Han, J and Heinemeyer, S and Hoecker, A and Holzbauer, JL and Hsu, S-C and Jaeger,
B and Janot, P and Kilian, W and Kogler, R and Kotwal, A and Langacker, P and Li, S and Linssen, L and Marx, M and Mattelaer, O and Metcalfe, J and Monig, K and Moortgat-Pick, G and Pleier, M-A and Pollard, C and Ramsey-Musolf, M and Rauch, M and Reuter, J and Rojo, J and Rominsky, M and Sakumoto, W and Schott, M and Schwinn, C and Sekulla, M and Stelzer, J and Torrence, E and Vicini, A and Wackeroth, D and Weiglein, G and Wilson,
G and Zeune, L},
Title = {Study of Electroweak Interactions at the Energy
Frontier},
Year = {2013},
Month = {October},
Abstract = {With the discovery of the Higgs boson, the spectrum of
particles in the Standard Model (SM) is complete. It is more
important than ever to perform precision measurements and to
test for deviations from SM predictions in the electroweak
sector. In this report, we investigate two themes in the
arena of precision electroweak measurements: the electroweak
precision observables (EWPOs) that test the particle content
and couplings in the SM and the minimal supersymmetric SM,
and the measurements involving multiple gauge bosons in the
final state which provide unique probes of the basic tenets
of electroweak symmetry breaking. Among the important EWPOs
we focus our discussion on M_W and sin^2 theta_eff^l, and on
anomalous quartic gauge couplings probed by triboson
production and vector boson scattering. We investigate the
thresholds of precision that need to be achieved in order to
be sensitive to new physics. We study the precision that can
be achieved at various facilities on these observables. We
discuss the calculational tools needed to predict SM rates
and distributions in order to perform these measurements at
the required precision. This report summarizes the work of
the Energy Frontier Precision Study of Electroweak
Interactions working group of the 2013 Community Summer
Study (Snowmass).},
Key = {fds362576}
}
@article{fds321079,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze,
G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Study of hard double-parton scattering in four-jet events in
pp collisions at √s=7 TeV with the ATLAS
experiment},
Journal = {Journal of High Energy Physics},
Volume = {2016},
Number = {11},
Publisher = {Springer Nature},
Year = {2016},
Month = {November},
url = {http://dx.doi.org/10.1007/JHEP11(2016)110},
Abstract = {Inclusive four-jet events produced in proton-proton
collisions at a centre-of-mass energy of s=7 TeV are
analysed for the presence of hard double-parton scattering
using data corresponding to an integrated luminosity of 37.3
pb−1, collected with the ATLAS detector at the LHC. The
contribution of hard double-parton scattering to the
production of four-jet events is extracted using an
artificial neural network, assuming that hard double-parton
scattering can be approximated by an uncorrelated overlaying
of dijet events. For events containing at least four jets
with transverse momentum pT ≥ 20 GeV and pseudorapidity
|η| ≤ 4.4, and at least one having pT ≥ 42.5 GeV, the
contribution of hard double-parton scattering is estimated
to be fDPS = 0.092− 0.011+ 0.005(stat.)− 0.037+
0.033(syst.). After combining this measurement with those of
the inclusive dijet and four-jet cross-sections in the
appropriate phase space regions, the effective
cross-section, σeff , was determined to be σeff = 14. 9−
1.0+ 1.2(stat.)− 3.8+ 5.1(syst.) mb. This result is
consistent within the quoted uncertainties with previous
measurements of σeff , performed at centre-of-mass energies
between 63 GeV and 8 TeV using various final states, and it
corresponds to 21− 6+ 7 % of the total inelastic
cross-section measured at s=7 TeV. The distributions of the
observables sensitive to the contribution of hard
double-parton scattering, corrected for detector effects,
are also provided.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP11(2016)110},
Key = {fds321079}
}
@article{fds307543,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allison, LJ and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai,
Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E and Arik, M and Armbruster, AJ},
Title = {Study of heavy-flavor quarks produced in association with
top-quark pairs at s =7TeV using the ATLAS
detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {April},
url = {http://dx.doi.org/10.1103/PhysRevD.89.072012},
Abstract = {Using a sample of dilepton top-quark pair (tt̄) candidate
events, a study is performed of the production of top-quark
pairs together with heavy-flavor (HF) quarks, the sum of
tt̄+b+X and tt̄+c+X, collectively referred to as tt̄+HF.
The data set used corresponds to an integrated luminosity of
4.7fb-1 of proton-proton collisions at a center-of-mass
energy of 7 TeV recorded by the ATLAS detector at the CERN
Large Hadron Collider. The presence of additional HF (b or
c) quarks in the tt̄ sample is inferred by looking for
events with at least three b-tagged jets, where two are
attributed to the b quarks from the tt̄ decays and the
third to additional HF production. The dominant background
to tt̄+HF in this sample is tt̄+jet events in which a
light-flavor jet is misidentified as a heavy-flavor jet. To
determine the heavy- and light-flavor content of the
additional b-tagged jets, a fit to the vertex mass
distribution of b-tagged jets in the sample is performed.
The result of the fit shows that 79±14(stat)±22(syst) of
the 105 selected extra b-tagged jets originate from HF
quarks, 3 standard deviations away from the hypothesis of
zero tt̄+HF production. The result for extra HF production
is quoted as a ratio (RHF) of the cross section for tt̄+HF
production to the cross section for tt̄ production with at
least one additional jet. Both cross sections are measured
in a fiducial kinematic region within the ATLAS acceptance.
RHF is measured to be [6.2±1.1(stat)±1.8(syst)]% for jets
with pT>25GeV and |η|<2.5, in agreement with the
expectations from Monte Carlo generators. © 2014 CERN, for
the ATLAS Collaboration.},
Doi = {10.1103/PhysRevD.89.072012},
Key = {fds307543}
}
@article{fds308152,
Author = {Acosta, and D, and others},
Title = {Study of jet shapes in inclusive jet production in p anti-p
collisions at s**(1/2) = 1.96-TeV},
Journal = {Phys. Rev.},
Volume = {D71},
Number = {11},
Pages = {112002},
Publisher = {American Physical Society (APS)},
Year = {2005},
url = {http://dx.doi.org/10.1103/PhysRevD.71.112002},
Abstract = {http://arxiv.org/abs/hep-ex/0505013},
Doi = {10.1103/PhysRevD.71.112002},
Key = {fds308152}
}
@article{fds307741,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdelalim, AA and Abdesselam,
A and Abdinov, O and Abi, B and Abolins, M and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Aderholz, M and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Åkesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Aliyev, M and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral, P and Amelung, C and Ammosov, VV and Amorim, A and Amorós, G and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, ML and Anduaga, XS and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi,
A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli,
F and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Archambault, JP and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnault, C},
Title = {Study of jets produced in association with a W boson in pp
collisions at √s=7TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.85.092002},
Abstract = {We report a study of final states containing a W boson and
hadronic jets, produced in proton-proton collisions at a
center-of-mass energy of 7 TeV. The data were collected with
the ATLAS detector at the CERN LHC and comprise the full
2010 data sample of 36pb-1. Cross sections are determined
using both the electron and muon decay modes of the W boson
and are presented as a function of inclusive jet
multiplicity, Njet, for up to five jets. At each
multiplicity, cross sections are presented as a function of
jet transverse momentum, the scalar sum of the transverse
momenta of the charged lepton, missing transverse momentum,
and all jets, the invariant mass spectra of jets, and the
rapidity distributions of various combinations of leptons
and final-state jets.},
Doi = {10.1103/PhysRevD.85.092002},
Key = {fds307741}
}
@article{fds312130,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and Devoto, F and D'Errico, M and Di Canto,
A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Study of orbitally excited B mesons and evidence for a new
Bπ resonance},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {90},
Number = {1},
Pages = {012013},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.90.012013},
Abstract = {Using the full CDF Run II data sample, we report evidence
for a new resonance, which we refer to as B(5970), found
simultaneously in the B0π+ and B+π- mass distributions
with a significance of 4.4 standard deviations. We further
report the first study of resonances consistent with
orbitally excited B+ mesons and an updated measurement of
the properties of orbitally excited B0 and Bs0 mesons. We
measure the masses and widths of all states, as well as the
relative production rates of the B1, B2*, and B(5970) states
and the branching fraction of the Bs2*0 state to either
B*+K- and B+K-. Furthermore, we measure the production rates
of the orbitally excited B0,+ states relative to the B0,+
ground state. The masses of the new B(5970) resonances are
5978±5(stat)±12(syst)MeV/c2 for the neutral state and
5961±5(stat)±12(syst)MeV/c2 for the charged state,
assuming that the resonance decays into Bπ final states.
The properties of the orbitally excited and the new
B(5970)0,+ states are compatible with isospin symmetry. ©
2014 American Physical Society.},
Doi = {10.1103/PhysRevD.90.012013},
Key = {fds312130}
}
@article{fds356721,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Afik, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ},
Title = {Study of ordered hadron chains with the ATLAS
detector},
Journal = {Physical Review D},
Volume = {96},
Number = {9},
Year = {2017},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.96.092008},
Abstract = {The analysis of the momentum difference between charged
hadrons in high-energy proton-proton collisions is performed
in order to study coherent particle production. The observed
correlation pattern agrees with a model of a helical QCD
string fragmenting into a chain of ground-state hadrons. A
threshold momentum difference in the production of adjacent
pairs of charged hadrons is observed, in agreement with
model predictions. The presence of low-mass hadron chains
also explains the emergence of charge-combination-dependent
two-particle correlations commonly attributed to
Bose-Einstein interference. The data sample consists of 190
μb-1 of minimum-bias events collected with proton-proton
collisions at a center-of-mass energy s=7 TeV in the early
low-luminosity data taking with the ATLAS detector at the
LHC.},
Doi = {10.1103/PhysRevD.96.092008},
Key = {fds356721}
}
@article{fds307801,
Author = {Aaltonen, T and Alon, R and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari,
G and Appel, JA and Apresyan, A and Arisawa, T and Artikov, A and Asaadi,
J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bauer, G and Bedeschi, F and Beecher, D and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Binkley, M and Bisello, D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Brisuda, A and Bromberg, C and Brucken, E and Bucciantonio, M and Budagov, J and Budd, HS and Budd, S and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calancha, C and Camarda, S and Campanelli,
M and Campbell, M and Canelli, F and Carls, B and Carlsmith, D and Carosi,
R and Carrillo, S and Carron, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho, K and Chokheli, D and Chou, JP and Chung, WH and Chung, YS and Ciobanu, CI and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuenca Almenar,
C and Cuevas, J and Culbertson, R},
Title = {Study of substructure of high transverse momentum jets
produced in proton-antiproton collisions at
√s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {85},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.85.091101},
Abstract = {A study of the substructure of jets with transverse momentum
greater than 400GeV/c produced in proton-antiproton
collisions at a center-of-mass energy of 1.96 TeV at the
Fermilab Tevatron Collider and recorded by the CDF II
detector is presented. The distributions of the jet mass,
angularity, and planar flow are measured for the first time
in a sample with an integrated luminosity of 5.95fb -1. The
observed substructure for high mass jets is consistent with
predictions from perturbative quantum chromodynamics. ©
2012 American Physical Society.},
Doi = {10.1103/PhysRevD.85.091101},
Key = {fds307801}
}
@article{fds347522,
Author = {Aaltonen, T and Albrow, M and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano,
A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld,
B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia,
A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli,
F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox,
DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto and A and Di Ruzza,
B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher,
R},
Title = {Study of the energy dependence of the underlying event in
proton-antiproton collisions},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {92},
Number = {9},
Year = {2015},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.92.092009},
Abstract = {We study charged particle production (pT>0.5 GeV/c,
|η|<0.8) in proton-antiproton collisions at total
center-of-mass energies s=300 GeV, 900 GeV, and 1.96 TeV. We
use the direction of the charged particle with the largest
transverse momentum in each event to define three regions of
η-φ space: "toward", "away", and "transverse." The average
number and the average scalar pT sum of charged particles in
the transverse region are sensitive to the modeling of the
"underlying event." The transverse region is divided into a
MAX and MIN transverse region, which helps separate the
"hard component" (initial and final-state radiation) from
the "beam-beam remnant" and multiple parton interaction
components of the scattering. The center-of-mass energy
dependence of the various components of the event is studied
in detail. The data presented here can be used to constrain
and improve QCD Monte Carlo models, resulting in more
precise predictions at the LHC energies of 13 and 14
TeV.},
Doi = {10.1103/PhysRevD.92.092009},
Key = {fds347522}
}
@article{fds356631,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adachi,
S and Adam, L and Adamczyk, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei,
C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos
Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S},
Title = {Study of the hard double-parton scattering contribution to
inclusive four-lepton production in pp collisions at √s=8
TeV with the ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {790},
Pages = {595-614},
Year = {2019},
Month = {January},
url = {http://dx.doi.org/10.1016/j.physletb.2019.01.062},
Abstract = {The inclusive production of four isolated charged leptons in
pp collisions is analysed for the presence of hard
double-parton scattering, using 20.2 fb−1 of data recorded
in the ATLAS detector at the LHC at centre-of-mass energy
s=8 TeV. In the four-lepton invariant-mass range of
80<m4ℓ<1000 GeV, an artificial neural network is used to
enhance the separation between single- and double-parton
scattering based on the kinematics of the four leptons in
the final state. An upper limit on the fraction of events
originating from double-parton scattering is determined at
95% confidence level to be fDPS=0.042, which results in an
estimated lower limit on the effective cross section at 95%
confidence level of 1.0 mb.},
Doi = {10.1016/j.physletb.2019.01.062},
Key = {fds356631}
}
@article{fds356713,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Abidi, SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov,
AV and Alberghi, GL and Albert, J and Albicocco, P and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei,
D and Dos Santos and SPA and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Ferraz, VA and Arce, ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster,
AJ and Armitage, LJ},
Title = {Study of the material of the ATLAS inner detector for Run 2
of the LHC},
Journal = {Journal of Instrumentation},
Volume = {12},
Number = {12},
Year = {2017},
Month = {December},
url = {http://dx.doi.org/10.1088/1748-0221/12/12/P12009},
Abstract = {The ATLAS inner detector comprises three different
sub-detectors: the pixel detector, the silicon strip
tracker, and the transition-radiation drift-tube tracker.
The Insertable B-Layer, a new innermost pixel layer, was
installed during the shutdown period in 2014, together with
modifications to the layout of the cables and support
structures of the existing pixel detector. The material in
the inner detector is studied with several methods, using a
low-luminosity s=13 TeV pp collision sample corresponding to
around 2.0 nb-1 collected in 2015 with the ATLAS experiment
at the LHC. In this paper, the material within the innermost
barrel region is studied using reconstructed hadronic
interaction and photon conversion vertices. For the forward
rapidity region, the material is probed by a measurement of
the efficiency with which single tracks reconstructed from
pixel detector hits alone can be extended with hits on the
track in the strip layers. The results of these studies have
been taken into account in an improved description of the
material in the ATLAS inner detector simulation, resulting
in a reduction in the uncertainties associated with the
charged-particle reconstruction efficiency determined from
simulation.},
Doi = {10.1088/1748-0221/12/12/P12009},
Key = {fds356713}
}
@article{fds356614,
Author = {Aaboud, M and Aad, G and Abbott, B and Abbott, DC and Abdinov, O and Abeloos, B and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adachi, S and Adam, L and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Aielli,
G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert, J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alhroob, M and Ali, B and Alimonti,
G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R and Arce, ATH and Ardell, RE and Arduh, FA},
Title = {Study of the rare decays of B s0 and B
0 mesons into muon pairs using data collected
during 2015 and 2016 with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2019},
Number = {4},
Year = {2019},
Month = {April},
url = {http://dx.doi.org/10.1007/JHEP04(2019)098},
Abstract = {A study of the decays B s0 → μ + μ − and B 0 → μ +
μ − has been performed using 26.3 fb −1 of 13 TeV LHC
proton-proton collision data collected with the ATLAS
detector in 2015 and 2016. Since the detector resolution in
μ + μ − invariant mass is comparable to the B s0 -B 0
mass difference, a single fit determines the signal yields
for both decay modes. This results in a measurement of the
branching fraction ℬ(Bs0→μ+μ−)=(3.2−1.0+1.1)×10−9
and an upper limit ℬ (B→ μ + μ − ) < 4.3 × 10 −
10 at 95% confidence level. The result is combined with the
Run 1 ATLAS result, yielding ℬ(Bs0→μ+μ−)=(2.8−0.7+0.8)×10−9
and ℬ (B→ μ + μ − ) < 2.1 × 10 − 10 at 95%
confidence level. The combined result is consistent with the
Standard Model prediction within 2.4 standard deviations in
the ℬ(B0→μ+μ−)−ℬ(Bs0→μ+μ−) plane.[Figure
not available: see fulltext.]},
Doi = {10.1007/JHEP04(2019)098},
Key = {fds356614}
}
@article{fds321094,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi,
P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow,
N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro,
F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley,
JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski,
R and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn,
D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch,
I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios,
C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka,
K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán,
SC and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura,
P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana,
S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelijn, R and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee,
A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A},
Title = {Study of the rare decays of [Formula: see text] and
[Formula: see text] into muon pairs from data collected
during the LHC Run 1 with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {9},
Pages = {513},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4338-8},
Abstract = {A study of the decays [Formula: see text] and [Formula: see
text] has been performed using data corresponding to an
integrated luminosity of 25 fb[Formula: see text] of 7 and
8 TeV proton-proton collisions collected with the ATLAS
detector during the LHC Run 1. For the [Formula: see text]
dimuon decay, an upper limit on the branching fraction is
set at [Formula: see text] at 95 % confidence level. For
[Formula: see text], the branching fraction [Formula: see
text] is measured. The results are consistent with the
Standard Model expectation with a <i>p</i> value of 4.8 %,
corresponding to 2.0 standard deviations.},
Doi = {10.1140/epjc/s10052-016-4338-8},
Key = {fds321094}
}
@article{fds346166,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da
Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle,
P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius,
C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana,
MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson,
N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi,
RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bieniek, SP and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Black,
CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boudreau,
J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark,
L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke,
S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth,
JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera
Urbán, S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet,
D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminal Armadans and R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero,
J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio,
A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Childers, JT and Chiodini,
G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi,
K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole, S and Colijn, AP and Collot,
J and Colombo, T and Compostella, G and Conde Muiño and P and Coniavitis,
E},
Title = {Study of the spin and parity of the Higgs boson in diboson
decays with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {10},
Pages = {476},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3685-1},
Abstract = {Studies of the spin, parity and tensor couplings of the
Higgs boson in the [Formula: see text], [Formula: see text]
and [Formula: see text] decay processes at the LHC are
presented. The investigations are based on [Formula: see
text] of <i>pp</i> collision data collected by the ATLAS
experiment at [Formula: see text] TeV and [Formula: see
text] TeV. The Standard Model (SM) Higgs boson hypothesis,
corresponding to the quantum numbers [Formula: see text], is
tested against several alternative spin scenarios, including
non-SM spin-0 and spin-2 models with universal and
non-universal couplings to fermions and vector bosons. All
tested alternative models are excluded in favour of the SM
Higgs boson hypothesis at more than 99.9 % confidence
level. Using the [Formula: see text] and [Formula: see text]
decays, the tensor structure of the interaction between the
spin-0 boson and the SM vector bosons is also investigated.
The observed distributions of variables sensitive to the
non-SM tensor couplings are compatible with the SM
predictions and constraints on the non-SM couplings are
derived.},
Doi = {10.1140/epjc/s10052-015-3685-1},
Key = {fds346166}
}
@booklet{Abachi97e,
Author = {Abachi, S and Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali, V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Borders, J and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and Di Loreto and G and Draper, P and Drinkard, J and Ducros, Y and Dudko, LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga,
MK and Featherly, J and Feher, S and Fein, D and Ferbel, T and Finocchiaro,
G and Fisk, HE},
Title = {Study of the ZZγ and Zγγ Couplings
in Z(νν)γ Production},
Journal = {Physical Review Letters},
Volume = {78},
Number = {19},
Pages = {3640-3645},
Publisher = {American Physical Society (APS)},
Year = {1997},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevLett.78.3640},
Abstract = {We have measured the ZZγ and ZZγ couplings by studying
13.1 pb−1 of pp¯→Etγ+ X data at √s = 1.8 TeV with
the Dø detector at the Fermilab Tevatron Collider. This is
the first study of hadronic Zγ production in the neutrino
decay channel. Combining this measurement with our previous
results using Z→ee and μμ yields the most stringent 95%
C.L. limits to date on anomalous couplings: |h30Z|<0.4,
|h40Z|<0.06 (λ=750 GeV. © 1997 The American Physical
Society.},
Doi = {10.1103/PhysRevLett.78.3640},
Key = {Abachi97e}
}
@article{fds346164,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso,
A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez,
B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos,
SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Auerbach, B and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balestri, T and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansil, HS and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat,
A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia,
M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker, M and Becker, S and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begel, M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Bensinger,
JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry,
T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Bieniek, SP and Biglietti, M and Bilbao De
Mendizabal and J and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd,
J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Breaden Madden and WD and Brendlinger, K and Brennan,
AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Buda, SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher,
D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan,
P and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro and R and Camarda, S and Camarri, P and Cameron, D and Caminada, LM and Caminal
Armadans, R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua,
M and Caputo, R and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charlton,
DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden,
A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen,
Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Cherkaoui El Moursli and R and Chernyatin, V and Cheu, E and Chevalier,
L and Chiarella, V and Childers, JT and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba,
J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Cleland, W and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Cole, B and Cole,
S and Colijn, AP and Collot, J and Colombo, T and Compostella, G and Conde
Muiño, P and Coniavitis, E and Connell, SH and Connelly,
IA},
Title = {Study of the [Formula: see text] and [Formula: see text]
decays with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Pages = {4},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3743-8},
Abstract = {The decays [Formula: see text] and [Formula: see text] are
studied with the ATLAS detector at the LHC using a dataset
corresponding to integrated luminosities of 4.9 and 20.6
fb[Formula: see text] of <i>pp</i> collisions collected at
centre-of-mass energies [Formula: see text] TeV and 8 TeV,
respectively. Signal candidates are identified through
[Formula: see text] and [Formula: see text] decays. With a
two-dimensional likelihood fit involving the [Formula: see
text] reconstructed invariant mass and an angle between the
[Formula: see text] and [Formula: see text] candidate
momenta in the muon pair rest frame, the yields of [Formula:
see text] and [Formula: see text], and the transverse
polarisation fraction in [Formula: see text] decay are
measured. The transverse polarisation fraction is determined
to be [Formula: see text], and the derived ratio of the
branching fractions of the two modes is [Formula: see text],
where the first error is statistical and the second is
systematic. Finally, a sample of [Formula: see text] decays
is used to derive the ratios of branching fractions
[Formula: see text] and [Formula: see text], where the third
error corresponds to the uncertainty of the branching
fraction of [Formula: see text] decay. The available
theoretical predictions are generally consistent with the
measurement.},
Doi = {10.1140/epjc/s10052-015-3743-8},
Key = {fds346164}
}
@article{fds307535,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Clark,
A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De Barbaro and P and Demortier, L and Deninno, M and D'Errico, M and Devoto, F and Di Canto,
A and Di Ruzza and B and Dittmann, JR and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A and Erbacher, R},
Title = {Study of top quark production and decays involving a tau
lepton at CDF and limits on a charged Higgs boson
contribution},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {89},
Number = {9},
Publisher = {American Physical Society (APS)},
Year = {2014},
Month = {May},
url = {http://dx.doi.org/10.1103/PhysRevD.89.091101},
Abstract = {We present an analysis of top-antitop quark production and
decay into a tau lepton, tau neutrino, and bottom quark
using data from 9fb-1 of integrated luminosity at the
Collider Detector at Fermilab. Dilepton events, where one
lepton is an energetic electron or muon and the other a
hadronically decaying tau lepton, originating from
proton-antiproton collisions at s=1.96TeV, are used. A
top-antitop quark production cross section of 8.1±2.1pb is
measured, assuming standard-model top quark decays. By
separately identifying for the first time the single-tau and
the ditau components, we measure the branching fraction of
the top quark into the tau lepton, tau neutrino, and bottom
quark to be (9.6±2.8)%. The branching fraction of top quark
decays into a charged Higgs boson and a bottom quark, which
would imply violation of lepton universality, is limited to
be less than 5.9% at a 95% confidence level [for
B(H-→τν̄)=1]. © 2014 American Physical
Society.},
Doi = {10.1103/PhysRevD.89.091101},
Key = {fds307535}
}
@article{fds348984,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baas, AE and Baca, MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagnaia, P and Bahmani, M and Bahrasemani, H and Baines, JT and Bajic, M and Baker, OK and Baldin, EM and Balek, P and Balli, F and Balunas, WK and Banas, E and Bandyopadhyay, A and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisits, M-S and Barkeloo, JT and Barklow, T and Barlow, N and Barnes,
SL and Barnett, BM and Barnett, RM and Barnovska-Blenessy, Z and Baroncelli, A and Barone, G and Barr, AJ and Barranco Navarro and L and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Beck, HC and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov,
VA and Bedognetti, M and Bee, CP and Beermann, TA and Begalli, M and Begel,
M and Behr, JK and Bell, AS and Bella, G and Bellagamba, L and Bellerive,
A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez, J and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Beringer, J and Berlendis, S and Bernard, NR and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella,
C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethani, A and Bethke, S and Bevan, AJ and Beyer, J and Bianchi, RM and Biebel, O and Biedermann, D and Bielski, R and Bierwagen, K and Biesuz, NV and Biglietti, M and Billoud, TRV and Bilokon, H and Bindi, M and Bingul, A and Bini, C and Biondi, S and Bisanz,
T and Bittrich, C and Bjergaard, DM and Black, CW and Black, JE and Black,
KM and Blair, RE and Blazek, T and Bloch, I and Blocker, C and Blue, A and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Boerner, D and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Boldyrev, AS and Bolz, AE and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Boscherini, D and Bosman, M and Bossio Sola and JD and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Boutle,
SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Breaden Madden and WD and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Briglin, DL and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans,
G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton,
JH and Bruckman de Renstrom and PA and Bruncko, D and Bruni, A and Bruni,
G and Bruni, LS and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burch, TJ and Burdin, S and Burgard, CD and Burger, AM and Burghgrave,
B and Burka, K and Burke, S and Burmeister, I and Burr, JTP and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Cabrera Urbán and S and Caforio, D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri, A and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvente Lopez and S and Calvet, D and Calvet, S and Calvet, TP and Camacho Toro and R and Camarda,
S and Camarri, P and Cameron, D and Caminal Armadans and R and Camincher,
C and Campana, S and Campanelli, M and Camplani, A and Campoverde, A and Canale, V and Cano Bret and M and Cantero, J and Cao, T and Capeans
Garrido, MDM and Caprini, I and Caprini, M and Capua, M and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, I and Carli, T and Carlino, G and Carlson, BT and Carminati, L and Carney, RMD and Caron, S and Carquin,
E and Carrá, S and Carrillo-Montoya, GD and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castelijn, R and Gimenez, VC and Castro,
NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro, E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Celebi, E and Ceradini, F and Cerda Alberich and L and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli,
A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, WS and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chau, CC and Chavez Barajas and CA and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, J and Chen, S and Chen, X and Chen, Y and Cheng,
HC and Cheng, HJ and Cheplakov, A and Cheremushkina, E and Cherkaoui El
Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chiu,
YH and Chizhov, MV and Choi, K and Chomont, AR and Chouridou, S and Chow,
YS and Christodoulou, V and Chu, MC and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocca, C and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C},
Title = {Study of W W γ and W Z γ production in p p collisions at s
= 8 TeV and search for anomalous quartic gauge couplings
with the ATLAS experiment.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {9},
Pages = {646},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5180-3},
Abstract = {This paper presents a study of W W γ and W Z γ triboson
production using events from proton-proton collisions at a
centre-of-mass energy of s = 8 TeV recorded with the ATLAS
detector at the LHC and corresponding to an integrated
luminosity of 20.2 fb - 1 . The W W γ production
cross-section is determined using a final state containing
an electron, a muon, a photon, and neutrinos ( e ν μ ν γ
). Upper limits on the production cross-section of the e ν
μ ν γ final state and the W W γ and W Z γ final states
containing an electron or a muon, two jets, a photon, and a
neutrino ( e ν j j γ or μ ν j j γ ) are also derived.
The results are compared to the cross-sections predicted by
the Standard Model at next-to-leading order in the
strong-coupling constant. In addition, upper limits on the
production cross-sections are derived in a fiducial region
optimised for a search for new physics beyond the Standard
Model. The results are interpreted in the context of
anomalous quartic gauge couplings using an effective field
theory. Confidence intervals at 95% confidence level are
derived for the 14 coupling coefficients to which W W γ and
W Z γ production are sensitive.},
Doi = {10.1140/epjc/s10052-017-5180-3},
Key = {fds348984}
}
@article{fds307924,
Author = {Aaltonen, and T, and others},
Title = {Studying the Underlying Event in Drell-Yan and High
Transverse Momentum Jet Production at the
Tevatron},
Journal = {Phys. Rev.},
Volume = {D82},
Number = {3},
Pages = {034001},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.82.034001},
Abstract = {http://arxiv.org/abs/1003.3146},
Doi = {10.1103/PhysRevD.82.034001},
Key = {fds307924}
}
@article{fds331390,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings, MAC and Cutts, D and Davis, GA and Davis, K and De, K and De Jong and SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros,
Y},
Title = {Subjet multiplicity of gluon and quark jets reconstructed
with the κ⊥ algorithm in pp̄
collisions},
Journal = {Physical Review D},
Volume = {65},
Number = {5},
Pages = {20},
Publisher = {American Physical Society (APS)},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.65.052008},
Abstract = {The DØ Collaboration has studied for the first time the
properties of hadron-collider jets reconstructed with a
successive-combination algorithm based on relative
transverse momenta (κ⊥) of energy clusters. Using the
standard value D = 1.0 of the jet-separation parameter in
the κ⊥ algorithm, we find that the pT of such jets is
higher than the ET of matched jets reconstructed with cones
of radius R = 0.7, by about 5 (8) GeV at pT ≈90 (240) GeV.
To examine internal jet structure, the κ⊥ algorithm is
applied within D = 0.5 jets to resolve any subjets. The
multiplicity of subjets in jet samples at √s = 1800 GeV
and 630 GeV is extracted separately for gluons (Mg) and
quarks (Mq), and the ratio of average subjet multiplicities
in gluon and quark jets is measured as (〈Mg〉-1)/(〈Mq〉-1)
= 1.84±0.15 (stat)±0.180.22 (syst). This ratio is in
agreement with the expectations from the HERWIG Monte Carlo
event generator and a resummation calculation, and with
observations in e+e- annihilations, and is close to the
naive prediction for the ratio of color charges of CA /CF =
9/4 = 2.25.},
Doi = {10.1103/PhysRevD.65.052008},
Key = {fds331390}
}
@article{fds347527,
Author = {Dwivedi, DA and Alasinga, S and Singhal, S and Malhotra, VK and Kotwal,
A},
Title = {Successful treatment of frostbite with hyperbaric oxygen
treatment.},
Journal = {Indian journal of occupational and environmental
medicine},
Volume = {19},
Number = {2},
Pages = {121-122},
Year = {2015},
Month = {May},
url = {http://dx.doi.org/10.4103/0019-5278.165336},
Doi = {10.4103/0019-5278.165336},
Key = {fds347527}
}
@article{fds313609,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A},
Title = {Summary of the ATLAS experiment’s sensitivity to
supersymmetry after LHC Run 1 — interpreted in the
phenomenological MSSM},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {10},
Publisher = {Springer Nature},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2015)134},
Abstract = {Abstract: A summary of the constraints from the ATLAS
experiment on R-parity-conserving supersymmetry is
presented. Results from 22 separate ATLAS searches are
considered, each based on analysis of up to 20.3 fb−1 of
proton-proton collision data at centre-of-mass energies of
s=7$$ \sqrt{s}=7 $$ and 8 TeV at the Large Hadron Collider.
The results are interpreted in the context of the
19-parameter phenomenological minimal supersymmetric
standard model, in which the lightest supersymmetric
particle is a neutralino, taking into account constraints
from previous precision electroweak and flavour measurements
as well as from dark matter related measurements. The
results are presented in terms of constraints on
supersymmetric particle masses and are compared to limits
from simplified models. The impact of ATLAS searches on
parameters such as the dark matter relic density, the
couplings of the observed Higgs boson, and the degree of
electroweak fine-tuning is also shown. Spectra for surviving
supersymmetry model points with low fine-tunings are
presented.[Figure not available: see fulltext.]},
Doi = {10.1007/JHEP10(2015)134},
Key = {fds313609}
}
@article{fds313604,
Author = {The ATLAS collaboration, and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio,
L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer,
A and Alvarez Gonzalez and B and Álvarez Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnold, H and Arratia, M and Arslan, O},
Title = {Summary of the searches for squarks and gluinos using √s =
8 TeV pp collisions with the ATLAS experiment at the
LHC},
Journal = {Journal of High Energy Physics},
Volume = {2015},
Number = {10},
Publisher = {Springer Nature},
Year = {2015},
Month = {October},
url = {http://dx.doi.org/10.1007/JHEP10(2015)054},
Abstract = {Abstract: A summary is presented of ATLAS searches for
gluinos and first- and second-generation squarks in final
states containing jets and missing transverse momentum, with
or without leptons or b-jets, in the s=8$$ \sqrt{s}=8 $$ TeV
data set collected at the Large Hadron Collider in 2012.
This paper reports the results of new interpretations and
statistical combinations of previously published analyses,
as well as a new analysis. Since no significant excess of
events over the Standard Model expectation is observed, the
data are used to set limits in a variety of models. In all
the considered simplified models that assume R-parity
conservation, the limit on the gluino mass exceeds 1150 GeV
at 95% confidence level, for an LSP mass smaller than 100
GeV. Furthermore, exclusion limits are set for left-handed
squarks in a phenomenological MSSM model, a minimal
Supergravity/Constrained MSSM model, R-parity-violation
scenarios, a minimal gauge-mediated supersymmetry breaking
model, a natural gauge mediation model, a non-universal
Higgs mass model with gaugino mediation and a minimal model
of universal extra dimensions.[Figure not available: see
fulltext.]},
Doi = {10.1007/JHEP10(2015)054},
Key = {fds313604}
}
@article{fds372387,
Author = {Aad, G and Abbott, B and Abbott, DC and Abeling, K and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Abusleme Hoffman and AC and Acharya, BS and Achkar, B and Adam
Bourdarios, C and Adamczyk, L and Adamek, L and Addepalli, SV and Adelman, J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov,
F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Albicocco, P and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alunno
Camelia, E and Alvarez Estevez and M and Alviggi, MG and Aly, M and Amaral
Coutinho, Y and Ambler, A and Amelung, C and Amerl, M and Ames, CG and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean,
SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov,
AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli,
M and Antrim, DJA and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo,
JA and Aparo, MA and Aperio Bella and L and Appelt, C and Aranzabal, N and Araujo Ferraz and V and Arcangeletti, C and Arce, ATH and Arena, E and Arguin, J-F and Argyropoulos, S and Arling, J-H and Armbruster, AJ and Arnaez, O and Arnold, H and Arrubarrena Tame and ZP and Artoni, G and Asada, H and Asai, K and Asai, S and Asbah, NA and Assahsah, J and Assamagan, K and Astalos, R and Atkin, RJ and Atkinson, M and Atlay, NB and Atmani, H and Atmasiddha, PA and Augsten, K and Auricchio, S and Auriol,
AD and Austrup, VA and Avner, G and Avolio, G and Axiotis, K and Ayoub, MK and Azuelos, G and Babal, D and Bachacou, H and Bachas, K and Bachiu, A and Backman, F and Badea, A and Bagnaia, P and Bahmani, M and Bailey, AJ and Bailey, VR and Baines, JT and Bakalis, C and Baker, OK and Bakker, PJ and Bakos, E and Bakshi Gupta and D and Balaji, S and Balasubramanian, R and Baldin, EM and Balek, P and Ballabene, E and Balli, F and Baltes, LM and Balunas, WK and Balz, J and Banas, E and Bandieramonte, M and Bandyopadhyay, A and Bansal, S and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barbour, G and Barends, KN and Barillari,
T and Barisits, M-S and Barklow, T and Barnett, RM and Baron, P and Baron
Moreno, DA and Baroncelli, A and Barone, G and Barr, AJ and Barranco
Navarro, L and Barreiro, F and Barreiro Guimarães da Costa and J and Barron, U and Barros Teixeira and MG and Barsov, S and Bartels, F and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Basan, A and Baselga, M and Bashta, I and Bassalat, A and Basso, MJ and Basson, CR and Bates, RL and Batlamous, S and Batley, JR and Batool, B and Battaglia,
M and Battulga, D and Bauce, M and Bauer, P and Bayirli, A and Beacham, JB and Beau, T and Beauchemin, PH and Becherer, F and Bechtle, P and Beck, HP and Becker, K and Beddall, AJ and Bednyakov, VA and Bee, CP and Beemster,
LJ and Beermann, TA and Begalli, M and Begel, M and Behera, A and Behr, JK and Beirao Da Cruz E Silva and C and Beirer, JF and Beisiegel, F and Belfkir, M and Bella, G and Bellagamba, L and Bellerive, A and Bellos,
P and Beloborodov, K and Belotskiy, K and Belyaev, NL and Benchekroun,
D and Bendebba, F and Benhammou, Y and Benjamin, DP and Benoit, M and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Bergeaas Kuutmann and E and Berger, N and Bergmann, B and Beringer, J and Berlendis, S and Bernardi, G and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Berthold, A and Bertram,
IA and Bethke, S and Betti, A and Bevan, AJ and Bhamjee, M and Bhatta, S and Bhattacharya, DS and Bhattarai, P and Bhopatkar, VS and Bi, R and Bianchi, RM and Biebel, O and Bielski, R and Biglietti, M and Billoud,
TRV and Bindi, M and Bingul, A and Bini, C and Biondi, S and Biondini, A and Birch-Sykes, CJ and Bird, GA and Birman, M and Bisanz, T and Bisceglie,
E and Biswas, D and Bitadze, A and Bjørke, K and Bloch, I and Blocker, C and Blue, A and Blumenschein, U and Blumenthal, J and Bobbink, GJ and Bobrovnikov, VS and Boehler, M and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bokan, P and Bold, T and Bomben, M and Bona, M and Boonekamp, M and Booth, CD and Borbély, AG and Borecka-Bielska, HM and Borgna, LS and Borissov, G and Bortoletto, D and Boscherini, D and Bosman, M and Bossio Sola and JD and Bouaouda, K and Bouchhar, N and Boudreau, J and Bouhova-Thacker, EV and Boumediene, D and Bouquet, R and Boveia, A and Boyd, J and Boye, D and Boyko, IR and Bracinik, J and Brahimi, N and Brandt, G and Brandt, O and Braren, F and Brau, B and Brau,
JE and Brendlinger, K and Brener, R and Brenner, L and Brenner, R and Bressler, S and Brickwedde, B and Britton, D and Britzger, D and Brock,
I and Brooijmans, G and Brooks, WK and Brost, E and Bruckler, TL and Bruckman de Renstrom and PA and Brüers, B and Bruncko, D and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Bugge, MK and Bulekov, O and Bullard, BA and Burdin, S and Burgard, CD and Burger, AM and Burghgrave, B and Burr, JTP and Burton, CD and Burzynski, JC and Busch,
EL and Büscher, V and Bussey, PJ and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Buxo Vazquez and CJ and Buzykaev,
AR and Cabras, G and Cabrera Urbán and S and Caforio, D and Cai, H and Cai,
Y and Cairo, VMM and Cakir, O and Calace, N and Calafiura, P and Calderini,
G and Calfayan, P and Callea, G and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Calvetti, M and Camacho Toro and R and Camarda, S and Camarero Munoz and D and Camarri, P and Camerlingo, MT and Cameron, D and Camincher, C and Campanelli, M and Camplani, A and Canale, V and Canesse, A and Cano Bret and M and Cantero, J and Cao, Y and Capocasa, F and Capua, M and Carbone, A and Cardarelli, R and Cardenas, JCJ and Cardillo, F and Carli, T and Carlino, G and Carlotto, JI and Carlson,
BT and Carlson, EM and Carminati, L and Carnesale, M and Caron, S and Carquin, E and Carrá, S and Carratta, G and Carrio Argos and F and Carter,
JWS and Carter, TM and Casado, MP and Casha, AF and Castiglia, EG and Castillo, FL and Castillo Garcia and L and Castillo Gimenez and V and Castro, NF and Catinaccio, A and Catmore, JR and Cavaliere, V and Cavalli, N and Cavasinni, V and Celebi, E and Celli, F and Centonze, MS and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cervelli, A and Cetin, SA and Chadi, Z and Chakraborty, D and Chala, M and Chan, J and Chan, WY and Chapman, JD and Chargeishvili, B and Charlton,
DG and Charman, TP and Chatterjee, M and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chen, A and Chen, B and Chen, C and Chen, H and Chen, J and Chen, S and Chen, SJ and Chen, X and Chen, Y and Cheng, CL and Cheng, HC and Cheong, S and Cheplakov, A and Cheremushkina, E and Cherepanova, E and Cherkaoui El Moursli and R and Cheu, E and Cheung, K and Chevalier, L and Chiarella, V and Chiarelli, G and Chiedde, N and Chiodini, G and Chisholm, AS and Chitan, A and Chitishvili, M and Chiu, YH and Chizhov,
MV and Choi, K and Chomont, AR and Chou, Y and Chow, EYS and Chowdhury, T and Christopher, LD and Chu, KL and Chu, MC and Chu, X and Chudoba, J and Chwastowski, JJ and Cieri, D and Ciesla, KM and Cindro, V and Ciocio, A and Cirotto, F and Citron, ZH and Citterio, M and Ciubotaru, DA and Ciungu,
BM and Clark, A and Clark, PJ and Clavijo Columbie,
JM},
Title = {Test of CP Invariance in Higgs Boson Vector-Boson-Fusion
Production Using the H→γγ Channel with the ATLAS
Detector.},
Journal = {Physical review letters},
Volume = {131},
Number = {6},
Pages = {061802},
Year = {2023},
Month = {August},
url = {http://dx.doi.org/10.1103/physrevlett.131.061802},
Abstract = {A test of CP invariance in Higgs boson production via
vector-boson fusion has been performed in the H→γγ
channel using 139 fb^{-1} of proton-proton collision
data at sqrt[s]=13 TeV collected by the ATLAS detector
at the LHC. The optimal observable method is used to probe
the CP structure of interactions between the Higgs boson and
electroweak gauge bosons, as described by an effective field
theory. No sign of CP violation is observed in the data.
Constraints are set on the parameters describing the
strength of the CP-odd component in the coupling between the
Higgs boson and the electroweak gauge bosons in two
effective field theory bases: d[over ˜] in the HISZ basis
and c_{HW[over ˜]} in the Warsaw basis. The results
presented are the most stringent constraints on CP violation
in the coupling between Higgs and weak bosons. The 95% C.L.
constraint on d[over ˜] is derived for the first time and
the 95% C.L. constraint on c_{HW[over ˜]} has been improved
by a factor of 5 compared to the previous
measurement.},
Doi = {10.1103/physrevlett.131.061802},
Key = {fds372387}
}
@article{fds349776,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alunno Camelia and E and Alvarez Estevez and M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Araque, JP and Araujo Ferraz and V and Araujo Pereira and R and Arcangeletti, C and Arce, ATH},
Title = {Test of CP invariance in vector-boson fusion production of
the Higgs boson in the H → ττ channel in
proton–proton collisions at [Formula presented] with the
ATLAS detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {805},
Year = {2020},
Month = {June},
url = {http://dx.doi.org/10.1016/j.physletb.2020.135426},
Abstract = {A test of CP invariance in Higgs boson production via
vector-boson fusion is performed in the H→ττ decay
channel. This test uses the Optimal Observable method and is
carried out using 36.1fb−1 of s=13TeV proton–proton
collision data collected by the ATLAS experiment at the LHC.
Contributions from CP-violating interactions between the
Higgs boson and electroweak gauge bosons are described by an
effective field theory, in which the parameter d˜ governs
the strength of CP violation. No sign of CP violation is
observed in the distributions of the Optimal Observable, and
d˜ is constrained to the interval [−0.090, 0.035] at the
68% confidence level (CL), compared to an expected interval
of d˜∈[−0.035,0.033] based upon the Standard Model
prediction. No constraints can be set on d˜ at 95% CL,
while an expected 95% CL interval of d˜∈[−0.21,0.15]
for the Standard Model hypothesis was expected.},
Doi = {10.1016/j.physletb.2020.135426},
Key = {fds349776}
}
@article{fds322002,
Author = {Aad, G and Abbott, B and Abdinov, O and Abdallah, J and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako,
K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro,
LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou,
Y and Noccioli, EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund,
OB and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bevan,
AJ and Bhimji, W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel,
O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas,
CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen,
H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chitan, A and Chizhov,
MV and Choi, K and Chomont, AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou,
Y},
Title = {Test of CP invariance in vector-boson fusion production of
the Higgs boson using the Optimal Observable method
in the ditau decay channel with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {12},
Pages = {658},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4499-5},
Abstract = {A test of CP invariance in Higgs boson production via
vector-boson fusion using the method of the <i>Optimal
Observable</i> is presented. The analysis exploits the decay
mode of the Higgs boson into a pair of [Formula: see text]
leptons and is based on 20.3 [Formula: see text] of
proton-proton collision data at [Formula: see text] =
8 [Formula: see text] collected by the ATLAS experiment at
the LHC. Contributions from CP-violating interactions
between the Higgs boson and electroweak gauge bosons are
described in an effective field theory framework, in which
the strength of CP violation is governed by a single
parameter [Formula: see text]. The mean values and
distributions of CP-odd observables agree with the
expectation in the Standard Model and show no sign of CP
violation. The CP-mixing parameter [Formula: see text] is
constrained to the interval [Formula: see text] at 68%
confidence level, consistent with the Standard Model
expectation of [Formula: see text].},
Doi = {10.1140/epjc/s10052-016-4499-5},
Key = {fds322002}
}
@article{fds357656,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adersberger, M and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal,
A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury,
K and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev,
M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia,
EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso,
S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen,
T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli,
CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim,
DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA},
Title = {Test of the universality of τ and μ lepton couplings in
W-boson decays with the ATLAS detector},
Journal = {Nature Physics},
Volume = {17},
Number = {7},
Pages = {813-818},
Publisher = {Springer Science and Business Media LLC},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1038/s41567-021-01236-w},
Abstract = {The standard model of particle physics encapsulates our best
current understanding of physics at the smallest scales. A
fundamental axiom of this theory is the universality of the
couplings of the different generations of leptons to the
electroweak gauge bosons. The measurement of the ratio of
the decay rate of W bosons to τ leptons and muons,
R(τ/μ), constitutes an important test of this axiom. Using
139 fb−1 of proton–proton collisions recorded with the
ATLAS detector at a centre-of-mass energy of 13 TeV, we
report a measurement of this quantity from di-leptonic tt¯
events where the top quarks decay into a W boson and a
bottom quark. We can distinguish muons originating from W
bosons and those originating from an intermediate τ lepton
through the muon transverse impact parameter and differences
in the muon transverse momentum spectra. The measured value
of R(τ/μ) is 0.992 ± 0.013 [± 0.007(stat) ±
0.011(syst)] and is in agreement with the hypothesis of
universal lepton couplings as postulated in the standard
model. This is the only such measurement from the Large
Hadron Collider, so far, and obtains twice the precision of
previous measurements.},
Doi = {10.1038/s41567-021-01236-w},
Key = {fds357656}
}
@article{fds313603,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox,
CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson,
R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de
Barbaro, P and de Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto,
F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, A and Evdokimov, VN and Farrington,
S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field, R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest, R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov, V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini, P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin, D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López,
O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald, MW and Guillemin, T and Guimaraes da
Costa, J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr, RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays, C and Hays, J and Head, T and Hebbeker, T and Hedin,
D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere, A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun,
SY and Jung, AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich, I and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg, J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster, M and Lannon, K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee, SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis, JD and Li, D and Li, H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour, J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega, J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett, J and Neu, C and Neustroev, P},
Title = {Tevatron Combination of Single-Top-Quark Cross Sections and
Determination of the Magnitude of the Cabibbo-Kobayashi-Maskawa
Matrix Element V_{tb}.},
Journal = {Physical review letters},
Volume = {115},
Number = {15},
Pages = {152003},
Year = {2015},
Month = {October},
ISSN = {0031-9007},
url = {http://dx.doi.org/10.1103/physrevlett.115.152003},
Abstract = {We present the final combination of CDF and D0 measurements
of cross sections for single-top-quark production in
proton-antiproton collisions at a center-of-mass energy of
1.96 TeV. The data correspond to total integrated
luminosities of up to 9.7 fb^{-1} per experiment. The
t-channel cross section is measured to be
σ_{t}=2.25_{-0.31}^{+0.29} pb. We also present the
combinations of the two-dimensional measurements of the s-
vs t-channel cross section. In addition, we give the
combination of the s+t channel cross section measurement
resulting in σ_{s+t}=3.30_{-0.40}^{+0.52} pb, without
assuming the standard model value for the ratio
σ_{s}/σ_{t}. The resulting value of the magnitude of the
top-to-bottom quark coupling is |V_{tb}|=1.02_{-0.05}^{+0.06},
corresponding to |V_{tb}|>0.92 at the 95%
C.L.},
Doi = {10.1103/physrevlett.115.152003},
Key = {fds313603}
}
@article{fds310289,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae,
T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett, JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto,
D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt,
O and Brigliadori, L and Brock, R and Bromberg, C and Bross, A and Brown,
D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto, G and Bussey, P and Buszello, CP and Butti, P and Buzatu, A and Calamba, A and Camacho-Pérez, E and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Casey, BCK and Castilla-Valdez, H and Castro, A and Catastini, P and Caughron, S and Cauz, D and Cavaliere, V and Cerri, A and Cerrito, L and Chakrabarti, S and Chan, KM and Chandra, A and Chapon, E and Chen, G and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Cho, K and Cho, SW and Choi, S and Chokheli, D and Choudhary, B and Cihangir, S and Claes, D and Clark, A and Clarke, C and Clutter, J and Convery, ME and Conway, J and Cooke, M and Cooper, WE and Corbo, M and Corcoran, M and Cordelli, M and Couderc, F and Cousinou, M-C and Cox,
CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson,
R and Cutts, D and Das, A and d'Ascenzo, N and Datta, M and Davies, G and de
Barbaro, P and de Jong, SJ and De La Cruz-Burelo and E and Déliot, F and Demina, R and Demortier, L and Deninno, M and Denisov, D and Denisov,
SP and D'Errico, M and Desai, S and Deterre, C and DeVaughan, K and Devoto,
F and Di Canto and A and Di Ruzza and B and Diehl, HT and Diesburg, M and Ding,
PF and Dittmann, JR and Dominguez, A and Donati, S and D'Onofrio, M and Dorigo, M and Driutti, A and Dubey, A and Dudko, LV and Duperrin, A and Dutt, S and Eads, M and Ebina, K and Edgar, R and Edmunds, D and Elagin, A and Ellison, J and Elvira, VD and Enari, Y and Erbacher, R and Errede, S and Esham, B and Evans, H and Evdokimov, VN and Farrington, S and Fauré, A and Feng, L and Ferbel, T and Fernández Ramos and JP and Fiedler, F and Field,
R and Filthaut, F and Fisher, W and Fisk, HE and Flanagan, G and Forrest,
R and Fortner, M and Fox, H and Franklin, M and Freeman, JC and Frisch, H and Fuess, S and Funakoshi, Y and Galloni, C and Garbincius, PH and Garcia-Bellido, A and García-González, JA and Garfinkel, AF and Garosi, P and Gavrilov, V and Geng, W and Gerber, CE and Gerberich, H and Gerchtein, E and Gershtein, Y and Giagu, S and Giakoumopoulou, V and Gibson, K and Ginsburg, CM and Ginther, G and Giokaris, N and Giromini,
P and Glagolev, V and Glenzinski, D and Gogota, O and Gold, M and Goldin,
D and Golossanov, A and Golovanov, G and Gomez, G and Gomez-Ceballos, G and Goncharov, M and González López and O and Gorelov, I and Goshaw, AT and Goulianos, K and Gramellini, E and Grannis, PD and Greder, S and Greenlee, H and Grenier, G and Gris, P and Grivaz, J-F and Grohsjean, A and Grosso-Pilcher, C and Group, RC and Grünendahl, S and Grünewald,
MW and Guillemin, T and Guimaraes da Costa and J and Gutierrez, G and Gutierrez, P and Hahn, SR and Haley, J and Han, JY and Han, L and Happacher, F and Hara, K and Harder, K and Hare, M and Harel, A and Harr,
RF and Harrington-Taber, T and Hatakeyama, K and Hauptman, JM and Hays,
C and Hays, J and Head, T and Hebbeker, T and Hedin, D and Hegab, H and Heinrich, J and Heinson, AP and Heintz, U and Hensel, C and Heredia-De
La Cruz and I and Herndon, M and Herner, K and Hesketh, G and Hildreth, MD and Hirosky, R and Hoang, T and Hobbs, JD and Hocker, A and Hoeneisen, B and Hogan, J and Hohlfeld, M and Holzbauer, JL and Hong, Z and Hopkins, W and Hou, S and Howley, I and Hubacek, Z and Hughes, RE and Husemann, U and Hussein, M and Huston, J and Hynek, V and Iashvili, I and Ilchenko, Y and Illingworth, R and Introzzi, G and Iori, M and Ito, AS and Ivanov, A and Jabeen, S and Jaffré, M and James, E and Jang, D and Jayasinghe, A and Jayatilaka, B and Jeon, EJ and Jeong, MS and Jesik, R and Jiang, P and Jindariani, S and Johns, K and Johnson, E and Johnson, M and Jonckheere,
A and Jones, M and Jonsson, P and Joo, KK and Joshi, J and Jun, SY and Jung,
AW and Junk, TR and Juste, A and Kajfasz, E and Kambeitz, M and Kamon, T and Karchin, PE and Karmanov, D and Kasmi, A and Kato, Y and Katsanos, I and Kaur, M and Kehoe, R and Kermiche, S and Ketchum, W and Keung, J and Khalatyan, N and Khanov, A and Kharchilava, A and Kharzheev, YN and Kilminster, B and Kim, DH and Kim, HS and Kim, JE and Kim, MJ and Kim, SH and Kim, SB and Kim, YJ and Kim, YK and Kimura, N and Kirby, M and Kiselevich,
I and Knoepfel, K and Kohli, JM and Kondo, K and Kong, DJ and Konigsberg,
J and Kotwal, AV and Kozelov, AV and Kraus, J and Kreps, M and Kroll, J and Kruse, M and Kuhr, T and Kumar, A and Kupco, A and Kurata, M and Kurča, T and Kuzmin, VA and Laasanen, AT and Lammel, S and Lammers, S and Lancaster,
M and Lannon, K and Latino, G and Lebrun, P and Lee, HS and Lee, JS and Lee,
SW and Lee, WM and Lei, X and Lellouch, J and Leo, S and Leone, S and Lewis,
JD and Li, D and Li, H and Li, L and Li, QZ and Lim, JK and Limosani, A and Lincoln, D and Linnemann, J and Lipaev, VV and Lipeles, E and Lipton, R and Lister, A and Liu, H and Liu, Q and Liu, T and Liu, Y and Lobodenko, A and Lockwitz, S and Loginov, A and Lokajicek, M and Lopes de Sa and R and Lucchesi, D and Lucà, A and Lueck, J and Lujan, P and Lukens, P and Luna-Garcia, R and Lungu, G and Lyon, AL and Lys, J and Lysak, R and Maciel, AKA and Madar, R and Madrak, R and Maestro, P and Magaña-Villalba, R and Malik, S and Malyshev, VL and Manca, G and Manousakis-Katsikakis, A and Mansour, J and Marchese, L and Margaroli, F and Marino, P and Martínez-Ortega, J and Matera, K and Mattson, ME and Mazzacane, A and Mazzanti, P and McCarthy, R and McGivern, CL and McNulty, R and Mehta, A and Mehtala, P and Meijer, MM and Melnitchouk, A and Menezes, D and Mercadante, PG and Merkin, M and Mesropian, C and Meyer, A and Meyer, J and Miao, T and Miconi, F and Mietlicki, D and Mitra, A and Miyake, H and Moed, S and Moggi, N and Mondal, NK and Moon, CS and Moore, R and Morello, MJ and Mukherjee, A and Mulhearn, M and Muller, T and Murat, P and Mussini, M and Nachtman, J and Nagai, Y and Naganoma, J and Nagy, E and Nakano, I and Napier, A and Narain, M and Nayyar, R and Neal, HA and Negret, JP and Nett, J and Neu, C and Neustroev, P and Nguyen, HT},
Title = {Tevatron constraints on models of the Higgs boson with
exotic spin and parity using decays to bottom-antibottom
quark pairs.},
Journal = {Physical review letters},
Volume = {114},
Number = {15},
Pages = {151802},
Year = {2015},
Month = {April},
url = {http://dx.doi.org/10.1103/physrevlett.114.151802},
Abstract = {Combined constraints from the CDF and D0 Collaborations on
models of the Higgs boson with exotic spin J and parity P
are presented and compared with results obtained assuming
the standard model value JP=0+. Both collaborations analyzed
approximately 10 fb(-) of proton-antiproton collisions
with a center-of-mass energy of 1.96 TeV collected at the
Fermilab Tevatron. Two models predicting exotic Higgs bosons
with JP=0- and JP=2+ are tested. The kinematic properties of
exotic Higgs boson production in association with a vector
boson differ from those predicted for the standard model
Higgs boson. Upper limits at the 95% credibility level on
the production rates of the exotic Higgs bosons, expressed
as fractions of the standard model Higgs boson production
rate, are set at 0.36 for both the JP=0- hypothesis and the
JP=2+ hypothesis. If the production rate times the branching
ratio to a bottom-antibottom pair is the same as that
predicted for the standard model Higgs boson, then the
exotic bosons are excluded with significances of 5.0
standard deviations and 4.9 standard deviations for the
JP=0- and JP=2+ hypotheses, respectively.},
Doi = {10.1103/physrevlett.114.151802},
Key = {fds310289}
}
@article{fds356677,
Author = {Aaltonen, T and Abazov, VM and Abbott, B and Acharya, BS and Adams, M and Adams, T and Agnew, JP and Alexeev, GD and Alkhazov, G and Alton, A and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Askew, A and Atkins, S and Auerbach, B and Augsten, K and Aurisano, A and Aushev, V and Aushev, Y and Avila, C and Azfar, F and Badaud, F and Badgett, W and Bae, T and Bagby, L and Baldin, B and Bandurin, DV and Banerjee, S and Barbaro-Galtieri, A and Barberis, E and Baringer, P and Barnes, VE and Barnett, BA and Barria, P and Bartlett,
JF and Bartos, P and Bassler, U and Bauce, M and Bazterra, V and Bean, A and Bedeschi, F and Begalli, M and Behari, S and Bellantoni, L and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Beri,
SB and Bernardi, G and Bernhard, R and Bertram, I and Besançon, M and Beuselinck, R and Bhat, PC and Bhatia, S and Bhatnagar, V and Bhatti, A and Bland, KR and Blazey, G and Blessing, S and Bloom, K and Blumenfeld, B and Bocci, A and Bodek, A and Boehnlein, A and Boline, D and Boos, EE and Borissov, G and Bortoletto, D and Borysova, M and Boudreau, J and Boveia, A and Brandt, A and Brandt, O and Brigliadori, L and Brochmann,
M and Brock, R and Bromberg, C and Bross, A and Brown, D and Brucken, E and Bu, XB and Budagov, J and Budd, HS and Buehler, M and Buescher, V and Bunichev, V and Burdin, S and Burkett, K and Busetto,
G},
Title = {Tevatron Run II combination of the effective leptonic
electroweak mixing angle},
Journal = {Physical Review D},
Volume = {97},
Number = {11},
Year = {2018},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.97.112007},
Abstract = {Drell-Yan lepton pairs produced in the process
pp→â.,"+â.,"-+X through an intermediate γ∗/Z boson
have an asymmetry in their angular distribution related to
the spontaneous symmetry breaking of the electroweak force
and the associated mixing of its neutral gauge bosons. The
CDF and D0 experiments have measured the effective-leptonic
electroweak mixing parameter sin2θefflept using electron
and muon pairs selected from the full Tevatron
proton-antiproton data sets collected in 2001-2011,
corresponding to 9-10 fb-1 of integrated luminosity. The
combination of these measurements yields the most precise
result from hadron colliders, sin2θefflept=0.23148±0.00033.
This result is consistent with, and approaches in precision,
the best measurements from electron-positron colliders. The
standard model inference of the on-shell electroweak mixing
parameter sin2θW, or equivalently the W-boson mass MW,
using the zfitter software package yields
sin2θW=0.22324±0.00033 or equivalently, MW=80.367±0.017
GeV/c2.},
Doi = {10.1103/PhysRevD.97.112007},
Key = {fds356677}
}
@article{fds359004,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Ali, S and Aliev, M and Alimonti,
G and Alison, J and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez,
MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Dos Santos and SPA and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders,
JK and Anderson, JT and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira,
RA},
Title = {The ATLAS fast TracKer system},
Journal = {Journal of Instrumentation},
Volume = {16},
Number = {7},
Year = {2021},
Month = {July},
url = {http://dx.doi.org/10.1088/1748-0221/16/07/P07006},
Abstract = {The ATLAS Fast TracKer (FTK) was designed to provide full
tracking for the ATLAS high-level trigger by using pattern
recognition based on Associative Memory (AM) chips and
fitting in high-speed field programmable gate arrays. The
tracks found by the FTK are based on inputs from all modules
of the pixel and silicon microstrip trackers. The as-built
FTK system and components are described, as is the online
software used to control them while running in the ATLAS
data acquisition system. Also described is the simulation of
the FTK hardware and the optimization of the AM pattern
banks. An optimization for long-lived particles with large
impact parameter values is included. A test of the FTK
system with the data playback facility that allowed the FTK
to be commissioned during the shutdown between Run 2 and Run
3 of the LHC is reported. The resulting tracks from part of
the FTK system covering a limited η-ϕ region of the
detector are compared with the output from the FTK
simulation. It is shown that FTK performance is in good
agreement with the simulation.},
Doi = {10.1088/1748-0221/16/07/P07006},
Key = {fds359004}
}
@article{fds362780,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek, L and Adelman,
J and Adiguzel, A and Adorni, S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmad, A and Ahmadov, F and Ahmed, WS and Ai,
X and Aielli, G and Akatsuka, S and Akbiyik, M and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi, GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob,
M and Ali, B and Ali, S and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Camelia, EA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and Anastopoulos, C and Andari, N and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Pozo, JAA and Aparo, MA and Bella, LA and Aranzabal, N and Ferraz, VA and Pereira, RA and Arcangeletti, C and Arce, ATH and Arguin, JF},
Title = {The ATLAS inner detector trigger performance in pp
collisions at 13 TeV during LHC Run 2},
Journal = {European Physical Journal C},
Volume = {82},
Number = {3},
Publisher = {Springer Science and Business Media LLC},
Year = {2022},
Month = {March},
url = {http://dx.doi.org/10.1140/epjc/s10052-021-09920-0},
Abstract = {The design and performance of the inner detector trigger for
the high level trigger of the ATLAS experiment at the Large
Hadron Collider during the 2016–2018 data taking period is
discussed. In 2016, 2017, and 2018 the ATLAS detector
recorded 35.6fb-1, 46.9fb-1, and 60.6fb-1 respectively of
proton–proton collision data at a centre-of-mass energy of
13 TeV. In order to deal with the very high interaction
multiplicities per bunch crossing expected with the 13 TeV
collisions the inner detector trigger was redesigned during
the long shutdown of the Large Hadron Collider from 2013
until 2015. An overview of these developments is provided
and the performance of the tracking in the trigger for the
muon, electron, tau and b-jet signatures is discussed. The
high performance of the inner detector trigger with these
extreme interaction multiplicities demonstrates how the
inner detector tracking continues to lie at the heart of the
trigger performance and is essential in enabling the ATLAS
physics programme.},
Doi = {10.1140/epjc/s10052-021-09920-0},
Key = {fds362780}
}
@article{fds308205,
Author = {Abbott, B and Abolins, M and Abramov, V and Acharya, BS and Adams, DL and Adams, M and Akimov, V and Alves, GA and Amos, N and Anderson, EW and Baarmand, MM and Babintsev, VV and Babukhadia, L and Baden, A and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Baringer, P and Bartlett, JF and Bassler, U and Bean, A and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar,
V and Bhattacharjee, M and Blazey, G and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Brandt, A and Breedon, R and Briskin,
G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler,
M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli, F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes,
D and Clark, AR and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl,
OI and Davis, K and De, K and del Signore, K and Demarteau, M and Denisov,
D and Denisov, SP and Diehl, HT and Diesburg, M and di Loreto, G and Doulas, S and Draper, P and Ducros, Y and Dudko, LV and Dugad, SR and Dyshkant, A and Edmunds, D and Ellison, J and Elvira, VD and Engelmann,
R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Estrada, J and Evans, H and Evdokimov, VN and Fahland, T and Feher, S and Fein,
D},
Title = {The bb̄ production cross section and angular correlations
in pp̄ collisions at √s = 1.8 TeV},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {487},
Number = {3-4},
Pages = {264-272},
Publisher = {Elsevier BV},
Year = {2000},
Month = {August},
url = {http://dx.doi.org/10.1016/S0370-2693(00)00844-3},
Abstract = {We present measurements of the bb̄ production cross section
and angular correlations using the DO detector at the
Fermilab Tevatron pp̄ Collider operating at √s = 1.8 TeV.
The b quark production cross section for |y(b)| < 1.0 and
p(T)/b > 6 GeV/c is extracted from single muon and dimuon
data samples. The results agree in shape with the
next-to-leading order QCD calculation of heavy flavor
production but are greater than the central values of these
predictions. The angular correlations between b and b̄
quarks, measured from the azimuthal opening angle between
their decay muons, also agree in shape with the
next-to-leading order QCD prediction. (C) 2000 Elsevier
Science B.V.},
Doi = {10.1016/S0370-2693(00)00844-3},
Key = {fds308205}
}
@article{fds310385,
Author = {ATLAS Collaboration, and Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acharya, BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke,
BMM and Allport, PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez
Gonzalez, B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amor Dos Santos and SP and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Andrieux, M-L and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki,
A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Aperio Bella and L and Apolle, R and Arabidze, G and Aracena,
I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Argyropoulos, S and Arik, E and Arik, M and Armbruster, AJ and Arnaez,
O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov,
D and Asai, S and Ask, S and Åsman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus
Mayes, J and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Balek, P and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barbaro Galtieri and A and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Behar Harpaz and S and Behera, PK and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar
Noccioli, E and Benitez Garcia and JA and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Berglund, E and Beringer, J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella, C and Bertin, A and Bertolucci, F and Besana, MI and Besjes,
GJ and Besson, N and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, CW and Black, KM and Blair, RE and Blanchard, J-B and Blanchot, G and Blazek,
T and Bloch, I and Blocker, C and Blocki, J and Blondel, A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta,
SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet, NM and Bomben, M and Bona, M and Boonekamp, M and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortfeldt,
J and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and Bruckman de Renstrom and PA and Bruncko, D and Bruneliere,
R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat, Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Büscher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Byszewski, M and Cabrera Urbán,
S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Camacho Toro and R and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli,
M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill,
R and Capasso, L and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda
Hernandez, AM and Castaneda-Miranda, E and Castillo Gimenez and V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron, S and Cavaliere,
V and Cavalleri, P and Cavalli, D and Cavalli-Sforza, M and Cavasinni,
V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman, JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Chavez
Barajas, CA and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheng, Y and Cheplakov, A and Cherkaoui El
Moursli and R and Chernyatin, V and Cheu, E and Cheung, SL and Chevalier,
L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov,
MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov,
A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citron, ZH and Citterio, M and Ciubancan, M},
Title = {The differential production cross section of the [Formula:
see text](1020) meson in [Formula: see text] = 7 TeV
[Formula: see text] collisions measured with the ATLAS
detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {74},
Number = {7},
Pages = {2895},
Year = {2014},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-014-2895-2},
Abstract = {A measurement is presented of the [Formula: see text]
production cross section at [Formula: see text] = 7 TeV
using [Formula: see text] collision data corresponding to an
integrated luminosity of 383 [Formula: see text], collected
with the ATLAS experiment at the LHC. Selection of [Formula:
see text](1020) mesons is based on the identification of
charged kaons by their energy loss in the pixel detector.
The differential cross section is measured as a function of
the transverse momentum, [Formula: see text], and rapidity,
[Formula: see text], of the [Formula: see text](1020) meson
in the fiducial region 500 [Formula: see text] 1200 MeV,
[Formula: see text] 0.8, kaon [Formula: see text] 230 MeV
and kaon momentum [Formula: see text] 800 MeV. The
integrated [Formula: see text]-meson production cross
section in this fiducial range is measured to be [Formula:
see text] = 570 [Formula: see text] 8 (stat) [Formula: see
text] 66 (syst) [Formula: see text] 20 (lumi) [Formula: see
text].},
Doi = {10.1140/epjc/s10052-014-2895-2},
Key = {fds310385}
}
@article{fds362572,
Author = {Assamagan, K and Chen, C-Y and Chou, JP and Curtin, D and Fedderke, MA and Gershtein, Y and He, X-G and Klute, M and Kozaczuk, J and Kotwal, A and Lowette, S and No, JM and Plehn, T and Qian, J and Ramsey-Musolf, M and Safonov, A and Shelton, J and Spannowsky, M and Su, S and Walker, DGE and Willocq, S and Winslow, P},
Title = {The Higgs Portal and Cosmology},
Year = {2016},
Month = {April},
Abstract = {Higgs portal interactions provide a simple mechanism for
addressing two open problems in cosmology: dark matter and
the baryon asymmetry. In the latter instance, Higgs portal
interactions may contain the ingredients for a strong first
order electroweak phase transition as well as new
CP-violating interactions as needed for electroweak
baryogenesis. These interactions may also allow for a viable
dark matter candidate. We survey the opportunities for
probing the Higgs portal as it relates to these questions in
cosmology at the LHC and possible future
colliders.},
Key = {fds362572}
}
@article{fds332353,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon,
TC and Baden, A and Baldin, B and Balm, PW and Banerjee, S and Barberis, E and Baringer, P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov,
VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cummings Crépé-Renaudin and MAC and Cutts,
D and Davis, GA and Davis, K and De, K and De Jong and SJ and Del Signore and K and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov, SP and Desai, S and Diehl, HT and Diesburg, M and Doulas, S and Ducros, Y and Dudko, LV},
Title = {The inclusive jet cross section in pp̄ collisions at √s =
1.8 TeV using the k⊥ algorithm},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {525},
Number = {3-4},
Pages = {211-218},
Publisher = {Elsevier BV},
Year = {2002},
Month = {January},
url = {http://dx.doi.org/10.1016/S0370-2693(01)01441-1},
Abstract = {The central inclusive jet cross section has been measured
using a successive-combination algorithm for reconstruction
of jets. The measurement uses 87.3 pb-1 of data collected
with the DØ detector at the Fermilab Tevatron pp̄ Collider
during 1994-1995. The cross section, reported as a function
of transverse momentum (pT > 60 GeV) in the central region
of pseudorapidity (|η| < 0.5), exhibits reasonable
agreement with next-to-leading order QCD predictions, except
at low pT where the agreement is marginal.},
Doi = {10.1016/S0370-2693(01)01441-1},
Key = {fds332353}
}
@article{fds321083,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and Abolins, M and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk,
L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei,
V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia,
M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Augsten, K and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas, AE and Baca,
MJ and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio,
EL and Barberis, D and Barbero, M and Barillari, T and Barklow, T and Barlow, N and Barnes, SL and Barnett, BM and Barnett, RM and Barnovska,
Z and Baroncelli, A and Barone, G and Barr, AJ and Navarro, LB and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton, AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates, RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer, F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin, PH and Bechtle, P and Beck, HP and Becker, K and Becker, M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bedognetti, M and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, AS and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Belyaev, NL and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli,
EB and Benitez, J and Garcia, JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford, L and Beretta, M and Berge, D and Kuutmann,
EB and Berger, N and Berghaus, F and Beringer, J and Berlendis, S and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta,
P and Bertella, C and Bertoli, G and Bertolucci, F and Bertram, IA and Bertsche, C and Bertsche, D and Besjes, GJ and Bylund, OB and Bessner,
M and Besson, N and Betancourt, C and Bethke, S and Bevan, AJ and Bhimji,
W and Bianchi, RM and Bianchini, L and Bianco, M and Biebel, O and Biedermann, D and Bielski, R and Biesuz, NV and Biglietti, M and De
Mendizabal, JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco,
JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein,
U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler, M and Boerner, D and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Bortfeldt, J and Bortoletto, D and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Sola, JDB and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene,
D and Bourdarios, C and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow,
TM and Britton, D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Broughton, JH and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Brunt, BH and Bruschi, M and Bruscino, N and Bryant, P and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burka, K and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Buzykaev, AR and Urbán, SC and Caforio, D and Cairo, VM and Cakir,
O and Calace, N and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet, S and Calvet, TP and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans, RC and Camincher, C and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli,
I and Carli, T and Carlino, G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez, VC and Castro, NF and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavallaro,
E and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerqueira, AS and Cerri, A and Cerrito,
L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chan, SK and Chan, YL and Chang, P and Chapman, JD and Charlton, DG and Chatterjee, A and Chau, CC and Barajas, CAC and Che, S and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, HJ and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini,
G and Chisholm, AS and Chitan, A and Chizhov, MV and Choi, K and Chomont,
AR and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, MR and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y},
Title = {The performance of the jet trigger for the ATLAS detector
during 2011 data taking.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {76},
Number = {10},
Pages = {526},
Year = {2016},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-016-4325-0},
Abstract = {The performance of the jet trigger for the ATLAS detector at
the LHC during the 2011 data taking period is described.
During 2011 the LHC provided proton-proton collisions with a
centre-of-mass energy of 7 TeV and heavy ion collisions
with a 2.76 TeV per nucleon-nucleon collision energy. The
ATLAS trigger is a three level system designed to reduce the
rate of events from the 40 MHz nominal maximum bunch
crossing rate to the approximate 400 Hz which can be
written to offline storage. The ATLAS jet trigger is the
primary means for the online selection of events containing
jets. Events are accepted by the trigger if they contain one
or more jets above some transverse energy threshold. During
2011 data taking the jet trigger was fully efficient for
jets with transverse energy above 25 GeV for triggers
seeded randomly at Level 1. For triggers which require a jet
to be identified at each of the three trigger levels, full
efficiency is reached for offline jets with transverse
energy above 60 GeV. Jets reconstructed in the final
trigger level and corresponding to offline jets with
transverse energy greater than 60 GeV, are reconstructed
with a resolution in transverse energy with respect to
offline jets, of better than 4 % in the central region and
better than 2.5 % in the forward direction.},
Doi = {10.1140/epjc/s10052-016-4325-0},
Key = {fds321083}
}
@article{fds375847,
Author = {Kotwal, AV},
Title = {The precision measurement of the W boson mass and its impact
on physics},
Journal = {Nature Reviews Physics},
Volume = {6},
Number = {3},
Pages = {180-193},
Publisher = {Springer Science and Business Media LLC},
Year = {2024},
Month = {March},
url = {http://dx.doi.org/10.1038/s42254-023-00682-0},
Abstract = {As a mediator of the weak nuclear force, the W boson
influences many properties of fundamental particles and
their interactions. Understanding the W boson as accurately
as possible, including knowing its mass, has been a priority
in particle physics for decades. In the past few years, in a
succession of increasing-precision measurements by multiple
experiments, a significant tension between the measured and
predicted mass has been documented by the CDF Collaboration.
Furthermore, smaller differences between different
measurements exist. Because the W boson mass provides a
window on new physics, a comparison between different
measurement techniques can inform the path to further
investigations. This Perspective article overviews the role
of the W boson mass in the Standard Model of Particle
Physics and its extensions, compares and contrasts its
measurement techniques and discusses prospects and future
directions.},
Doi = {10.1038/s42254-023-00682-0},
Key = {fds375847}
}
@article{fds308106,
Author = {Abazov, VM and Abbott, B and Abolins, M and Acharya, BS and Adams, DL and Adams, M and Adams, T and Agelou, M and Agram, JL and Ahmed, SN and Ahn,
SH and Ahsan, M and Alexeev, GD and Alkhazov, G and Alton, A and Alverson,
G and Alves, GA and Anastasoaie, M and Andeen, T and Anderson, JT and Anderson, S and Andrieu, B and Angstadt, R and Anosov, V and Arnoud, Y and Arov, M and Askew, A and Åsman, B and Assis Jesus and ACS and Atramentov,
O and Autermann, C and Avila, C and Babukhadia, L and Bacon, TC and Badaud,
F and Baden, A and Baffioni, S and Bagby, L and Baldin, B and Balm, PW and Banerjee, P and Banerjee, S and Barberis, E and Bardon, O and Barg, W and Bargassa, P and Baringer, P and Barnes, C and Barreto, J and Bartlett,
JF and Bassler, U and Bhattacharjee, M and Baturitsky, MA and Bauer, D and Bean, A and Baumbaugh, B and Beauceron, S and Begalli, M and Beaudette,
F and Begel, M and Bellavance, A and Beri, SB and Bernardi, G and Bernhard,
R and Bertram, I and Besançon, M and Besson, A and Beuselinck, R and Beutel, D and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Binder, M and Biscarat, C and Bishoff, A and Black, KM and Blackler, I and Blazey, G and Blekman, F and Blessing, S and Bloch, D and Blumenschein, U and Bockenthien, E and Bodyagin, V and Boehnlein, A and Boeriu, O and Bolton, TA and Bonamy, P and Bonifas, D and Borcherding, F and Borissov,
G and Bos, K and Bose, T and Boswell, C and Bowden, M and Brandt, A and Briskin, G and Brock, R and Brooijmans, G and Bross,
A},
Title = {The upgraded DØ detector},
Journal = {Nuclear Instruments and Methods in Physics Research, Section
A: Accelerators, Spectrometers, Detectors and Associated
Equipment},
Volume = {565},
Number = {2},
Pages = {463-537},
Publisher = {Elsevier BV},
Year = {2006},
Month = {September},
url = {http://dx.doi.org/10.1016/j.nima.2006.05.248},
Abstract = {The DØ experiment enjoyed a very successful data-collection
run at the Fermilab Tevatron collider between 1992 and 1996.
Since then, the detector has been upgraded to take advantage
of improvements to the Tevatron and to enhance its physics
capabilities. We describe the new elements of the detector,
including the silicon microstrip tracker, central fiber
tracker, solenoidal magnet, preshower detectors, forward
muon detector, and forward proton detector. The
uranium/liquid-argon calorimeters and central muon detector,
remaining from Run I, are discussed briefly. We also present
the associated electronics, triggering, and data acquisition
systems, along with the design and implementation of
software specific to DØ. © 2006 Elsevier B.V. All rights
reserved.},
Doi = {10.1016/j.nima.2006.05.248},
Key = {fds308106}
}
@article{fds326606,
Author = {Kotwal, AV},
Title = {The W Boson mass measurement},
Volume = {26},
Pages = {185-200},
Booktitle = {The Standard Theory of Particle Physics: Essays to Celebrate
CERN's 60th Anniversary},
Publisher = {World Scientific},
Year = {2016},
Month = {October},
ISBN = {9789814733502},
url = {http://dx.doi.org/10.1142/9878},
Abstract = {The measurement of the W boson mass has been growing in
importance as its precision has improved, along with the
precision of other electroweak observables and the top quark
mass. Over the last decade, the measurement of the W boson
mass has been led at hadron colliders. Combined with the
precise measurement of the top quark mass at hadron
colliders, the W boson mass helped to pin down the mass of
the Standard Model Higgs boson through its induced radiative
correction on theW boson mass. With the discovery of the
Higgs boson and the measurement of its mass, the electroweak
sector of the Standard Model is over-constrained. Increasing
the precision of the W boson mass probes new physics at the
TeV-scale. We summarize an extensive Tevatron (1984-2011)
program to measure the W boson mass at the CDF and DØ
experiments. We highlight the recent Tevatron measurements
and prospects for the final Tevatron measurements.},
Doi = {10.1142/9878},
Key = {fds326606}
}
@article{fds346212,
Author = {Prakash, J and Kotwal, A and Prabhu, H},
Title = {Therapeutic and prophylactic utility of the memory-enhancing
drug donepezil hydrochloride on cognition of patients
undergoing electroconvulsive therapy: a randomized
controlled trial.},
Journal = {The journal of ECT},
Volume = {22},
Number = {3},
Pages = {163-168},
Year = {2006},
Month = {September},
url = {http://dx.doi.org/10.1097/01.yct.0000230365.81368.2d},
Abstract = {<h4>Objectives</h4>Substantial progress has been made in
identifying how the treatment parameters used in
electroconvulsive therapy (ECT) impact its cognitive side
effects. However, there is limited information regarding the
role of memory enhancers in post-ECT cognitive disturbances.
We evaluated the therapeutic and prophylactic efficacy of
the memory-enhancing drug donepezil hydrochloride on
cognition of patients undergoing ECT.<h4>Methods</h4>A
triple blind (the study subjects, clinician assessing the
cognition, and the data analyst were unaware of subject
allocation for trial assessment) randomized controlled trial
was carried out in a General Hospital Psychiatry Unit.
Subjects were randomized into 2 groups. One group received
ECT with placebo, whereas the other group received ECT and
donepezil (a memory-enhancing drug). Study participants were
assessed in post-ECT period to analyze cognitive deficits
and to compare the differences in 2 groups, as regards
recovery of various aspects of cognition.<h4>Results</h4>The
post-ECT recovery of various components of cognition was
more rapid in patients using donepezil as compared to those
not given donepezil (P < 0.05).<h4>Conclusions</h4>This
significant improvement in recovery time among patients
receiving donepezil bears therapeutic implication in
immediate post-ECT cognitive deficits.},
Doi = {10.1097/01.yct.0000230365.81368.2d},
Key = {fds346212}
}
@article{fds308264,
Author = {O'Donnell, JM and Kotwal, A and Fortune, HT},
Title = {Three-state mixing among 0+ states in even Cd
isotopes.},
Journal = {Physical review. C, Nuclear physics},
Volume = {38},
Number = {5},
Pages = {2047-2051},
Year = {1988},
Month = {November},
url = {http://dx.doi.org/10.1103/physrevc.38.2047},
Abstract = {Ratios of (t,p) transfer intensities to 0+ states in the
cadmium isotopes have been analyzed using a three-state
mixing model. The data allows determination of the degree of
mixing of the rotational (intruder) state into the
zero-phonon and two-phonon 0+ states. The three lowest 0+
states are found to be relatively pure and the intruder
state lies above the two-phonon state in the heavier
isotopes. © 1988 The American Physical Society.},
Doi = {10.1103/physrevc.38.2047},
Key = {fds308264}
}
@article{fds313583,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Khalek, SA and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan, T and Akesson, TPA and Akimoto, G and Akimov, AV and Alam, MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov, IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Allbrooke, BMM and Allport,
PP and Allwood-Spiers, SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Gonzalez, BA and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Anger,
P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aoun, S and Bella, LA and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, J-F and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni, G and Arutinov, D and Asai, S and Asfandiyarov, R and Ask, S and Asman, B and Asquith, L and Assamagan, K and Astbury, A and Atkinson, M and Aubert, B and Auge, E and Augsten, K and Aurousseau, M and Avolio, G and Avramidou, R and Axen, D and Azuelos, G and Azuma, Y and Baak, MA and Baccaglioni, G and Bacci, C and Bach, AM and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Badescu, E and Bagnaia, P and Bahinipati, S and Bai, Y and Bailey, DC and Bain, T and Baines, JT and Baker, OK and Baker, MD and Baker, S and Banas, E and Banerjee, P and Banerjee, S and Banfi, D and Bangert, A and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Galtieri, AB and Barber, T and Barberio, EL and Barberis, D and Barbero, M and Bardin, DY and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett,
BM and Barnett, RM and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Barrillon, P and Bartoldus, R and Barton, AE and Bartsch, V and Basye, A and Bates, RL and Batkova, L and Batley, JR and Battaglia, A and Battistin, M and Bauer, F and Bawa, HS and Beale, S and Beau, T and Beauchemin, PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, AK and Becker, S and Beckingham, M and Becks, KH and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee,
CP and Beemster, LJ and Begel, M and Harpaz, SB and Beimforde, M and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellina, F and Bellomo, M and Belloni, A and Beloborodova, O and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia, JAB and Benjamin, DP and Benoit, M and Bensinger, JR and Benslama, K and Bentvelsen, S and Berge, D and Kuutmann, EB and Berger, N and Berghaus, F and Berglund, E and Beringer,
J and Bernat, P and Bernhard, R and Bernius, C and Berry, T and Bertella,
C and Bertin, A and Bertolucci, F and Besana, MI and Besjes, GJ and Besson,
N and Bethke, S and Bhimji, W and Bianchi, RM and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biscarat, C and Bittner, B and Black, KM and Blair, RE and Blanchard,
J-B and Blanchot, G and Blazek, T and Blocker, C and Blocki, J and Blondel,
A and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VB and Bocchetta, SS and Bocci, A and Boddy, CR and Boehler, M and Boek, J and Boelaert, N and Bogaerts, JA and Bogdanchikov, A and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Bolnet,
NM and Bomben, M and Bona, M and Boonekamp, M and Booth, CN and Bordoni, S and Borer, C and Borisov, A and Borissov, G and Borjanovic, I and Borri, M and Borroni, S and Bortolotto, V and Bos, K and Boscherini, D and Bosman, M and Boterenbrood, H and Bouchami, J and Boudreau, J and Bouhova-Thacker,
EV and Boumediene, D and Bourdarios, C and Bousson, N and Boveia, A and Boyd, J and Boyko, IR and Bozovic-Jelisavcic, I and Bracinik, J and Branchini, P and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Bremer, J and Brendlinger, K and Brenner, R and Bressler, S and Britton,
D and Brochu, FM and Brock, I and Brock, R and Broggi, F and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brown, G and Brown, H and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Brunet, S and Bruni, A and Bruni, G and Bruschi, M and Buanes, T and Buat,
Q and Bucci, F and Buchanan, J and Buchholz, P and Buckingham, RM and Buckley, AG and Buda, SI and Budagov, IA and Budick, B and Buescher, V and Bugge, L and Bulekov, O and Bundock, AC and Bunse, M and Buran, T and Burckhart, H and Burdin, S and Burgess, T and Burke, S and Busato, E and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Buttar, CM and Butterworth, JM and Buttinger, W and Cabrera Urban and S and Caforio, D and Cakir, O and Calafiura, P and Calderini, G and Calfayan, P and Calkins,
R and Caloba, LP and Caloi, R and Calvet, D and Calvet, S and Toro, RC and Camarri, P and Cameron, D and Caminada, LM and Caminal Armadans and R and Campana, S and Campanelli, M and Canale, V and Canelli, F and Canepa, A and Cantero, J and Cantrill, R and Capasso, L and Garrido, MDMC and Caprini,
I and Caprini, M and Capriotti, D and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati, L and Caron, B and Caron, S and Carquin, E and Montoya, GDC and Carter, AA and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Cascella, M and Caso, C and Castaneda Hernandez and AM and Castaneda-Miranda, E and Castillo
Gimenez, V and Castro, NF and Cataldi, G and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caughron,
S and Cavaliere, V and Cavalleri, P and Cavalli, D and Cavalli-Sforza,
M and Cavasinni, V and Ceradini, F and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cetin, SA and Chafaq, A and Chakraborty,
D and Chalupkova, I and Chan, K and Chang, P and Chapleau, B and Chapman,
JD and Chapman, JW and Chareyre, E and Charlton, DG and Chavda, V and Barajas, CAC and Cheatham, S and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, S and Chen, X and Chen, Y and Cheplakov, A and El Moursli and RC and Chernyatin,
V and Cheu, E and Cheung, SL and Chevalier, L and Chiefari, G and Chikovani, L and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choudalakis, G and Chouridou, S and Christidi, IA and Christov, A and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocca, C and Ciocio, A and Cirilli, M and Cirkovic, P and Citterio, M and Ciubancan,
M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, B and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J},
Title = {Time-dependent angular analysis of the decay
Bs0 → J/ψφ and
extraction of ΔΓs and the
CP-violating weak phase φs by
ATLAS},
Journal = {JOURNAL OF HIGH ENERGY PHYSICS},
Volume = {2012},
Number = {12},
Year = {2012},
ISSN = {1126-6708},
url = {http://dx.doi.org/10.1007/JHEP12(2012)072},
Abstract = {A measurement of B0s → J /ψφ decay parameters, including
the CP -violating weak phase φ s and the decay width
difference ΔΓ s is reported, using 4.9 fb-1 of integrated
luminosity collected in 2011 by the ATLAS detector from LHC
pp collisions at a centre-of-mass energy √s = 7 TeV. The
mean decay width Γ s and the transversity amplitudes |A
0(0)|2 and |A arap;(0)|2 are also measured. The values
reported for these parameters are: φs = 0.22 ± 0.41 (stat)
± 0.10 (syst) rad} ΔΓ s = 0.053 ± 0.021 (stat) ± 0.010
(sast) ps-1 Γ s = 0.677 ± 0.007 (stat) ± 0.004 (sast)
ps-1 |A0(0)|2 = 0.528 ± 0.006 (stat) ± 0.009 (sast)
|A0(0)|2 = 0.220 ± 0.008 (stat) ± 0.007 (sast) where the
values quoted for φ s and ΔΓ s correspond to the solution
compatible with the external measurements to which the
strong phase δ ⊥ is constrained and where ΔΓ s is
constrained to be positive. The fraction of S-wave KK or f 0
contamination through the decays B0s→ J /ψK +
K-}}\left({{f-0}} \right)}} \right.} is measured as well and
is found to be consistent with zero. Results for φ s and
ΔΓ s are also presented as 68%, 90% and 95% likelihood
contours, which show agreement with Standard Model
expectations.[Figure not available: see fulltext.] © 2012
CERN for the benefit of the ATLAS collaboration.},
Doi = {10.1007/JHEP12(2012)072},
Key = {fds313583}
}
@article{fds375336,
Author = {Aad, G and Abbott, B and Abeling, K and Abicht, NJ and Abidi, SH and Aboulhorma, A and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Adam Bourdarios and C and Adamczyk, L and Addepalli, SV and Addison, MJ and Adelman, J and Adiguzel, A and Adye, T and Affolder, AA and Afik, Y and Agaras, MN and Agarwala, J and Aggarwal, A and Agheorghiesei, C and Ahmad, A and Ahmadov, F and Ahmed, WS and Ahuja, S and Ai, X and Aielli, G and Aikot, A and Ait Tamlihat and M and Aitbenchikh, B and Aizenberg, I and Akbiyik, M and Åkesson, TPA and Akimov, AV and Akiyama, D and Akolkar, NN and Al Khoury and K and Alberghi, GL and Albert,
J and Albicocco, P and Albouy, GL and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, F and Algren, M and Alhroob, M and Ali, B and Ali, HMJ and Ali, S and Alibocus,
SW and Aliev, M and Alimonti, G and Alkakhi, W and Allaire, C and Allbrooke, BMM and Allen, JF and Allendes Flores and CA and Allport, PP and Aloisio, A and Alonso, F and Alpigiani, C and Alvarez Estevez and M and Alvarez Fernandez and A and Alves Cardoso and M and Aly, M and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Amelung, C and Amerl, M and Ames,
CG and Amidei, D and Amor Dos Santos and SP and Amos, KR and Ananiev, V and Anastopoulos, C and Andeen, T and Anders, JK and Andrean, SY and Andreazza, A and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antipov, E and Antonelli, M and Anulli, F and Aoki, M and Aoki, T and Aparisi Pozo and JA and Aparo, MA and Aperio Bella and L and Appelt, C},
Title = {Tools for estimating fake/non-prompt lepton backgrounds with
the ATLAS detector at the LHC},
Journal = {Journal of Instrumentation},
Volume = {18},
Number = {11},
Pages = {T11004-T11004},
Publisher = {IOP Publishing},
Year = {2023},
Month = {November},
url = {http://dx.doi.org/10.1088/1748-0221/18/11/T11004},
Abstract = {Measurements and searches performed with the ATLAS detector
at the CERN LHC often involve signatures with one or more
prompt leptons. Such analyses are subject to
'fake/non-prompt' lepton backgrounds, where either a hadron
or a lepton from a hadron decay or an electron from a photon
conversion satisfies the prompt-lepton selection criteria.
These backgrounds often arise within a hadronic jet because
of particle decays in the showering process, particle
misidentification or particle interactions with the detector
material. As it is challenging to model these processes with
high accuracy in simulation, their estimation typically uses
data-driven methods. Three methods for carrying out this
estimation are described, along with their implementation in
ATLAS and their performance.},
Doi = {10.1088/1748-0221/18/11/T11004},
Key = {fds375336}
}
@article{fds308098,
Author = {Abulencia, and A, and others},
Title = {Top quark mass measurement from dilepton events at CDF
II},
Journal = {Phys. Rev. Lett.},
Volume = {96},
Number = {15},
Pages = {152002},
Year = {2006},
url = {http://dx.doi.org/10.1103/physrevlett.96.152002},
Abstract = {We report a measurement of the top quark mass using events
collected by the CDF II Detector from p anti-p collisions at
s**(1/2) = 1.96 TeV at the Fermilab Tevatron. We calculate a
likelihood function for the top mass in events that are
consistent with t anti-t --> b-bar l- nu-bar_l bl'+ nu'_l
decays. The likelihood is formed as the convolution of the
leading-order matrix element and detector resolution
functions. The joint likelihood is the product of
likelihoods for each of 33 events collected in 340 pb-1 of
integrated luminosity, yielding a top quark mass M_t = 165.2
+/- 6.1(stat.) +/- 3.4(syst.) GeV/c2. This first application
of a matrix-element technique to tt-bar --> bl+ nu_l b-bar
l'- nu-bar_l' decays gives the most precise single
measurement of M_t in dilepton events. Combined with other
CDF Run II measurements using dilepton events, we measure
M_t = 167.9 +/- 5.2(stat.) +/- 3.7(syst.)
GeV/c2.},
Doi = {10.1103/physrevlett.96.152002},
Key = {fds308098}
}
@article{fds308121,
Author = {Abulencia, and A, and others},
Title = {Top quark mass measurement from dilepton events at CDF II
with the matrix-element method},
Journal = {Phys. Rev.},
Volume = {D74},
Number = {3},
Pages = {032009},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.74.032009},
Abstract = {We describe a measurement of the top quark mass using events
with two charmed leptons collected by the CDF II detector
from p anti-p collisions with s**(1/2) = 1.96 TeV at the
Fermilab Tevatron. The likelihood in top mass is calculated
for each event by convoluting the leading order matrix
element describing qqbar --> t anti-t --> b l nu_l b-bar l'
nu_l' with detector resolution functions. The presence of
background events in the data sample is modeled using
similar calculations involving the matrix elements for major
background processes. In a data sample with integrated
luminosity of 340 pb-1, we observe 33 candidate events and
measure M_top = 165.2 +/- 6.1(stat.) +/- 3.4(syst.) GeV/c2.
This measurement represents the first application of this
method to events with two charged leptons and is the most
precise single measurement of the top quark mass in this
channel.},
Doi = {10.1103/PhysRevD.74.032009},
Key = {fds308121}
}
@article{fds307894,
Author = {Aaltonen, and T, and others},
Title = {Top Quark Mass Measurement in the $lepton+jets$ Channel
Using a Matrix Element Method and in situ Jet Energy
Calibration},
Journal = {Phys. Rev. Lett.},
Volume = {105},
Number = {25},
Pages = {252001},
Publisher = {American Physical Society},
Year = {2010},
Month = {December},
url = {http://dx.doi.org/10.1103/PhysRevLett.105.252001},
Abstract = {A precision measurement of the top quark mass m(t) is
obtained using a sample of tt events from pp collisions at
the Fermilab Tevatron with the CDF II detector. Selected
events require an electron or muon, large missing transverse
energy, and exactly four high-energy jets, at least one of
which is tagged as coming from a b quark. A likelihood is
calculated using a matrix element method with quasi-Monte
Carlo integration taking into account finite detector
resolution and jet mass effects. The event likelihood is a
function of m(t) and a parameter Δ(JES) used to calibrate
the jet energy scale in situ. Using a total of 1087 events
in 5.6 fb(-1) of integrated luminosity, a value of
m(t)=173.0 ± 1.2 GeV/c(2) is measured.},
Doi = {10.1103/PhysRevLett.105.252001},
Key = {fds307894}
}
@article{fds307980,
Author = {Aaltonen, T and others},
Title = {Top quark mass measurement in the lepton plus jets channel
using a modified matrix element method},
Journal = {Phys. Rev. D},
Volume = {79},
Number = {7},
Pages = {072001},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.072001},
Abstract = {We report a measurement of the top quark mass, mt, obtained
from pp̄ collisions at s=1.96TeV at the Fermilab Tevatron
using the CDF II detector. We analyze a sample corresponding
to an integrated luminosity of 1.9fb-1. We select events
with an electron or muon, large missing transverse energy,
and exactly four high-energy jets in the central region of
the detector, at least one of which is tagged as coming from
a b quark. We calculate a signal likelihood using a matrix
element integration method, where the matrix element is
modified by using effective propagators to take into account
assumptions on event kinematics. Our event likelihood is a
function of mt and a parameter JES (jet energy scale) that
determines in situ the calibration of the jet energies. We
use a neural network discriminant to distinguish signal from
background events. We also apply a cut on the peak value of
each event likelihood curve to reduce the contribution of
background and badly reconstructed events. Using the 318
events that pass all selection criteria, we find
mt=172.7±1.8(stat+JES) ±1.2(syst)GeV/c2. © 2009 The
American Physical Society.},
Doi = {10.1103/PhysRevD.79.072001},
Key = {fds307980}
}
@article{fds307979,
Author = {Aaltonen, T and others},
Title = {Top quark mass measurement in the tt̅ all hadronic channel
using a matrix element technique in pp̅ collisions at
sqrt[s] =1.96 TeV},
Journal = {Physical Review D},
Volume = {79},
Number = {7},
Pages = {072010},
Publisher = {APS},
Year = {2009},
url = {http://dx.doi.org/10.1103/PhysRevD.79.072010},
Abstract = {We present a measurement of the top quark mass in the all
hadronic channel (tt̅ →bb̅ q1q̅ 2q3q̅ 4) using
943 pb-1 of pp̅ collisions at sqrt[s]=1.96 TeV
collected at the CDF II detector at Fermilab (CDF). We apply
the standard model production and decay matrix element (ME)
to tt̅ candidate events. We calculate per-event probability
densities according to the ME calculation and construct
template models of signal and background. The scale of the
jet energy is calibrated using additional templates formed
with the invariant mass of pairs of jets. These templates
form an overall likelihood function that depends on the top
quark mass and on the jet energy scale (JES). We estimate
both by maximizing this function. Given 72 observed events,
we measure a top quark mass of 171.1 ± 3.7(stat+JES)
± 2.1(syst) GeV/c2. The combined uncertainty on
the top quark mass is 4.3 GeV/c2.},
Doi = {10.1103/PhysRevD.79.072010},
Key = {fds307979}
}
@article{fds307925,
Author = {Aaltonen, and T, and others},
Title = {Top Quark Mass Measurement using $m_{T2}$ in the Dilepton
Channel at CDF},
Journal = {Phys. Rev.},
Volume = {D81},
Number = {3},
Pages = {031102},
Publisher = {American Physical Society (APS)},
Year = {2010},
url = {http://dx.doi.org/10.1103/PhysRevD.81.031102},
Abstract = {http://arxiv.org/abs/0911.2956},
Doi = {10.1103/PhysRevD.81.031102},
Key = {fds307925}
}
@article{fds307869,
Author = {Aaltonen, and T, and al, E},
Title = {Top quark mass measurement using the template method at
{CDF}},
Journal = {Phys. Rev. D},
Volume = {83},
Number = {11},
Pages = {111101},
Publisher = {American Physical Society},
Year = {2011},
Month = {June},
url = {http://dx.doi.org/10.1103/PhysRevD.83.111101},
Abstract = {We present a measurement of the top quark mass in the
lepton+jets and dilepton channels of tt̄ decays using the
data sample corresponding to an integrated luminosity of
5.6fb-1 of pp̄ collisions at Tevatron with √s=1.96TeV,
collected with the CDF II detector. We construct templates
of two reconstructed top quark masses from different
jets-to-quarks combinations and the invariant mass of two
jets from the W decays in the lepton+jets channel, and a
reconstructed top quark mass and mT2, a variable related to
the transverse mass in events with two missing particles, in
the dilepton channel. The simultaneous fit of the templates
from signal and background events in the lepton+jets and
dilepton channels to the data yields a measured top quark
mass of Mtop=172.1±1.1(stat)±0. 9(syst)GeV/c2. © 2011
American Physical Society.},
Doi = {10.1103/PhysRevD.83.111101},
Key = {fds307869}
}
@article{fds308107,
Author = {Abulencia, and A, and others},
Title = {Top quark mass measurement using the template method in the
lepton + jets channel at CDF II},
Journal = {Phys. Rev.},
Volume = {D73},
Number = {3},
Pages = {032003},
Publisher = {American Physical Society (APS)},
Year = {2006},
url = {http://dx.doi.org/10.1103/PhysRevD.73.032003},
Abstract = {This article presents a measurement of the top quark mass
using the CDF II detector at Fermilab. Colliding beams of
protons and anti-protons at Fermilab's Tevatron (s**(1/2) =
1.96 TeV) produce top/anti-top pairs, which decay to W+ W-
bb-bar; events are selected where one W decays to hadrons,
and the other W decays to either e or mu plus a neutrino.
The data sample corresponds to an integrated luminosity of
approximately 318 pb-1. A total of 165 tt-bar events are
separated into four subsamples based on jet transverse
energy thresholds and the number of b jets identified by
reconstructing a displaced vertex. In each event, the
reconstructed top quark invariant mass is determined by
minimizing a chi2 for the overconstrained kinematic system.
At the same time, the mass of the hadronically decaying W
boson is measured in the same event sample. The observed W
boson mass provides an in situ improvement in the
determination of the hadronic jet energy scale, JES. A
simultaneous likelihood fit of the reconstructed top quark
masses and the W boson invariant masses in the data sample
to distributions from simulated signal and background events
gives a top quark mass of 173.5+3.7_-3.6(stat. + JES) +/-
1.3 (other syst.) GeV/c2, or 173.5+3.9_-3.8
GeV/c2.},
Doi = {10.1103/PhysRevD.73.032003},
Key = {fds308107}
}
@article{fds307592,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and D'Errico, M and Devoto,
F and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Top-quark mass measurement in events with jets and missing
transverse energy using the full CDF data
set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {88},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {July},
url = {http://dx.doi.org/10.1103/PhysRevD.88.011101},
Abstract = {We present a measurement of the top-quark mass using the
full data set of Tevatron √s=1.96 TeV proton-antiproton
collisions recorded by the CDF II detector, corresponding to
an integrated luminosity of 8.7 fb-1. The analysis uses
events with one semileptonic t or t̄ decay, but without
detection of the electron or muon. We select events with
significant missing transverse energy and multiple jets. We
veto events containing identified electrons or muons. We
obtain distributions of the top-quark masses and the
invariant mass of the two jets from W-boson decays from data
and compare these to templates derived from signal and
background samples to extract the top-quark mass and the
energy scale of the calorimeter jets with in situ
calibration. A likelihood fit of the templates from signal
and background events to the data yields the top-quark mass,
Mtop=173.93±1.64(stat)±0. 87(syst) GeV/c2. This result is
the most precise measurement to date of the mass of the top
quark in this event topology. © 2013 American Physical
Society.},
Doi = {10.1103/PhysRevD.88.011101},
Key = {fds307592}
}
@article{fds356739,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz,
H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, M and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi,
A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli,
F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O},
Title = {Top-quark mass measurement in the all-hadronic tt¯ decay
channel at √s=8 TeV with the ATLAS detector},
Journal = {Journal of High Energy Physics},
Volume = {2017},
Number = {9},
Year = {2017},
Month = {September},
url = {http://dx.doi.org/10.1007/JHEP09(2017)118},
Abstract = {The top-quark mass is measured in the all-hadronic
top-antitop quark decay channel using proton-proton
collisions at a centre-of-mass energy of s=8 TeV with the
ATLAS detector at the CERN Large Hadron Collider. The data
set used in the analysis corresponds to an integrated
luminosity of 20.2 fb −1 . The large multi-jet background
is modelled using a data-driven method. The top-quark mass
is obtained from template fits to the ratio of the three-jet
to the dijet mass. The three-jet mass is obtained from the
three jets assigned to the top quark decay. From these three
jets the dijet mass is obtained using the two jets assigned
to the W boson decay. The top-quark mass is measured to be
173.72 ± 0.55 (stat.) ± 1.01 (syst.) GeV.[Figure not
available: see fulltext.].},
Doi = {10.1007/JHEP09(2017)118},
Key = {fds356739}
}
@article{fds307831,
Author = {Aaltonen, TEA},
Title = {Top-Quark Mass Measurement Using Events with Missing
Transverse Energy and Jets at CDF},
Journal = {Phys. Rev. Lett.},
Volume = {107},
Number = {23},
Pages = {232002},
Publisher = {American Physical Society},
Year = {2011},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevLett.107.232002},
Abstract = {We present a measurement of the top-quark mass using a
sample of $t\bar{t}$ events in 5.7 fb-1 of integrated
luminosity from $p\bar{p}$ collisions at the Fermilab
Tevatron with $\sqrt{s}=1.96$ TeV and collected by the
CDF II Detector. We select events having large missing
transverse energy, and four, five, or six jets with at least
one jet tagged as coming from a b quark, and reject events
with identified charged leptons. This analysis considers
events from the semileptonic tt̅ decay channel, including
events that contain tau leptons. The measurement is based on
a multidimensional template method. We fit the data to
signal templates of varying top-quark masses and background
templates, and measure a top-quark mass of Mtop=$172.32\pm
2.4$(stat)$\pm 1.0$(syst) GeV/c2.},
Doi = {10.1103/PhysRevLett.107.232002},
Key = {fds307831}
}
@article{fds347509,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Aben, R and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman,
J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson, TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Verzini, MJA and Aleksa,
M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Alkire, SP and Allbrooke, BMM and Allport, PP and Aloisio, A and Alonso, A and Alonso,
F and Alpigiani, C and Altheimer, A and Gonzalez, BA and Piqueras, DÁ and Alviggi, MG and Amadio, BT and Amako, K and Coutinho, YA and Amelung, C and Amidei, D and Santos, SPAD and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonelli, M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Bella, LA and Arabidze, G and Arai, Y and Araque, JP and Arce,
ATH and Arduh, FA and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni, G and Artz, S and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos,
R and Atkinson, M and Atlay, NB and Augsten, K and Aurousseau, M and Avolio, G and Axen, B and Ayoub, MK and Azuelos, G and Baak, MA and Baas,
AE and Baca, MJ and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Baldin, EM and Balek, P and Balestri, T and Balli, F and Balunas, WK and Banas, E and Banerjee, S and Bannoura, AAE and Barak, L and Barberio, EL and Barberis, D and Barbero, M and Barillari,
T and Barisonzi, M and Barklow, T and Barlow, N and Barnes, SL and Barnett,
BM and Barnett, RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and da Costa, JBG and Bartoldus, R and Barton,
AE and Bartos, P and Basalaev, A and Bassalat, A and Basye, A and Bates,
RL and Batista, SJ and Batley, JR and Battaglia, M and Bauce, M and Bauer,
F and Bawa, HS and Beacham, JB and Beattie, MD and Beau, T and Beauchemin,
PH and Beccherle, R and Bechtle, P and Beck, HP and Becker, K and Becker,
M and Beckingham, M and Becot, C and Beddall, AJ and Beddall, A and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bender, M and Bendtz, K and Benekos, N and Benhammou, Y and Noccioli, EB and Garcia,
JAB and Benjamin, DP and Bensinger, JR and Bentvelsen, S and Beresford,
L and Beretta, M and Berge, D and Kuutmann, EB and Berger, N and Berghaus,
F and Beringer, J and Bernard, C and Bernard, NR and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bylund, OB and Bessner, M and Besson, N and Betancourt,
C and Bethke, S and Bevan, AJ and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Biedermann, D and Biesuz, NV and Biglietti, M and De Mendizabal and JB and Bilokon, H and Bindi, M and Binet, S and Bingul, A and Bini, C and Biondi, S and Bjergaard, DM and Black, CW and Black, JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blanco, JE and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Blunier, S and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock, C and Boehler,
M and Bogaerts, JA and Bogavac, D and Bogdanchikov, AG and Bohm, C and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson, N and Boutle, SK and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau,
JE and Braun, HM and Madden, WDB and Brendlinger, K and Brennan, AJ and Brenner, L and Brenner, R and Bressler, S and Bristow, TM and Britton,
D and Britzger, D and Brochu, FM and Brock, I and Brock, R and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and de Renstrom, PAB and Bruncko, D and Bruneliere, R and Bruni, A and Bruni, G and Bruschi, M and Bruscino, N and Bryngemark, L and Buanes, T and Buat, Q and Buchholz, P and Buckley, AG and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov, O and Bullock, D and Burckhart, H and Burdin, S and Burgard, CD and Burghgrave, B and Burke, S and Burmeister,
I and Busato, E and Büscher, D and Büscher, V and Bussey, P and Butler,
JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu, A and Buzykaev, AR and Urbán, SC and Caforio,
D and Cairo, VM and Cakir, O and Calace, N and Calafiura, P and Calandri,
A and Calderini, G and Calfayan, P and Caloba, LP and Calvet, D and Calvet,
S and Toro, RC and Camarda, S and Camarri, P and Cameron, D and Armadans,
RC and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Bret, MC and Cantero, J and Cantrill, R and Cao, T and Garrido, MDMC and Caprini, I and Caprini, M and Capua, M and Caputo, R and Carbone, RM and Cardarelli, R and Cardillo, F and Carli, T and Carlino,
G and Carminati, L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino,
M and Casper, DW and Castaneda-Miranda, E and Castelli, A and Gimenez,
VC and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Alberich, LC and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chan, YL and Chang, P and Chapman,
JD and Charlton, DG and Chau, CC and Barajas, CAC and Che, S and Cheatham,
S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen,
S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cheremushkina, E and Moursli, RCE and Chernyatin, V and Cheu, E and Chevalier, L and Chiarella, V and Chiarelli, G and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Choi, K and Chouridou, S and Chow, BKB and Christodoulou, V and Chromek-Burckhart, D and Chudoba, J and Chuinard, AJ and Chwastowski,
JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Cinca, D and Cindro, V and Cioara, IA and Ciocio, A and Cirotto, F and Citron, ZH and Ciubancan, M and Clark, A and Clark, BL and Clark, PJ and Clarke, RN and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L and Cogan, JG and Colasurdo, L and Cole, B and Cole, S and Colijn,
AP},
Title = {Topological cell clustering in the ATLAS calorimeters and
its performance in LHC Run 1.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {77},
Number = {7},
Pages = {490},
Year = {2017},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-017-5004-5},
Abstract = {The reconstruction of the signal from hadrons and jets
emerging from the proton-proton collisions at the Large
Hadron Collider (LHC) and entering the ATLAS calorimeters is
based on a three-dimensional topological clustering of
individual calorimeter cell signals. The cluster formation
follows cell signal-significance patterns generated by
electromagnetic and hadronic showers. In this, the
clustering algorithm implicitly performs a topological noise
suppression by removing cells with insignificant signals
which are not in close proximity to cells with significant
signals. The resulting <i>topological cell clusters</i> have
shape and location information, which is exploited to apply
a local energy calibration and corrections depending on the
nature of the cluster. Topological cell clustering is
established as a well-performing calorimeter signal
definition for jet and missing transverse momentum
reconstruction in ATLAS.},
Doi = {10.1140/epjc/s10052-017-5004-5},
Key = {fds347509}
}
@article{fds346206,
Author = {Priya, R and Kotwal, A and Qadeer, I},
Title = {Toward an ecosocial epidemiological approach to goiter and
other iodine deficiency disorders: a case study of India's
technocratic program for universal iodization of
salt.},
Journal = {International journal of health services : planning,
administration, evaluation},
Volume = {39},
Number = {2},
Pages = {343-362},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.2190/hs.39.2.g},
Abstract = {The program of universal salt iodization (USI) was
intensified in the 1990s. Unfortunately, a recent World
Health Organization review finds that there was a global
increase of 31.7 percent in total goiter rate from 1993 to
2003. However, the WHO review places only 1 country as
severely, 13 as moderately, and 40 as mildly deficient in
populations' iodine nutrition, and places 43 countries at
optimal, 24 at high, and 5 at excessive levels of iodine
nutrition. Thus, it is imperative to weigh the benefits and
risks of intensifying USI further. The WHO review places
India in the category of "adequate" iodine nutrition, but in
2005 the Government of India promulgated a universal ban on
sale of non-iodized salt, calling iodine deficiency
disorders (IDDs) a major public health problem. This article
attempts to understand these contradictions and weigh the
benefits and costs of USI. Based on a review of studies
since the 1920s, the authors reconstruct the evolution of
IDD control in India. Conceptual and methodological
limitations challenge the evidence base and rationale of
stricter implementation of USI now. Finding evidence for its
negative impact, the authors recommend a reexamination of
the USI strategy and propose a safer, people-centered,
ecosocial epidemiological approach rather than a universal
legal ban.},
Doi = {10.2190/hs.39.2.g},
Key = {fds346206}
}
@article{fds346188,
Author = {Kotwal, A},
Title = {Training-associated injuries among Armed Forces
trainees.},
Journal = {Medical journal, Armed Forces India},
Volume = {68},
Number = {2},
Pages = {106-107},
Year = {2012},
Month = {April},
url = {http://dx.doi.org/10.1016/s0377-1237(12)60015-x},
Doi = {10.1016/s0377-1237(12)60015-x},
Key = {fds346188}
}
@article{fds356552,
Author = {Aad, G and Abbott, B and Abbott, DC and Abud, AA and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Bourdarios, CA and Adamczyk, L and Adamek,
L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni, S and Adye,
T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras, MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Verzini, MJA and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, F and Alpigiani, C and Alshehri, AA and Estevez, MA and Alviggi, MG and Coutinho, YA and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Santos, SPAD and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Pozo, JAA and Bella, LA and Araque, JP and Ferraz, VA and Pereira,
RA and Arcangeletti, C and Arce, ATH and Arduh, FA},
Title = {Transverse momentum and process dependent azimuthal
anisotropies in √sNN=8.16 TeV p+Pb collisions with the
ATLAS detector},
Journal = {European Physical Journal C},
Volume = {80},
Number = {1},
Year = {2020},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-020-7624-4},
Abstract = {The azimuthal anisotropy of charged particles produced in
sNN=8.16 TeV p+Pb collisions is measured with the ATLAS
detector at the LHC. The data correspond to an integrated
luminosity of 165 nb - 1 that was collected in 2016.
Azimuthal anisotropy coefficients, elliptic v2 and
triangular v3, extracted using two-particle correlations
with a non-flow template fit procedure, are presented as a
function of particle transverse momentum (pT) between 0.5
and 50 GeV. The v2 results are also reported as a function
of centrality in three different particle pT intervals. The
results are reported from minimum-bias events and
jet-triggered events, where two jet pT thresholds are used.
The anisotropies for particles with pT less than about
2 GeV are consistent with hydrodynamic flow expectations,
while the significant non-zero anisotropies for pT in the
range 9–50 GeV are not explained within current
theoretical frameworks. In the pT range 2–9 GeV, the
anisotropies are larger in minimum-bias than in
jet-triggered events. Possible origins of these effects,
such as the changing admixture of particles from hard
scattering and the underlying event, are
discussed.},
Doi = {10.1140/epjc/s10052-020-7624-4},
Key = {fds356552}
}
@article{fds307811,
Author = {Aaltonen, T and Alvarez González and B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'ascenzo, N and Datta, M and De
Barbaro, P and Dell'orso, M and Demortier, L and Deninno, M and Devoto,
F and D'errico, M},
Title = {Transverse momentum cross section of e +e
- pairs in the Z-boson region from pp̄
collisions at √s=1.96TeV},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {September},
url = {http://dx.doi.org/10.1103/PhysRevD.86.052010},
Abstract = {The transverse momentum cross section of e +e - pairs in the
Z-boson mass region of 66-116GeV/c2 is precisely measured
using Run II data corresponding to 2.1fb -1 of integrated
luminosity recorded by the Collider Detector at Fermilab.
The cross section is compared with two quantum chromodynamic
calculations. One is a fixed-order perturbative calculation
at O(αs2), and the other combines perturbative predictions
at high transverse momentum with the gluon resummation
formalism at low transverse momentum. Comparisons of the
measurement with calculations show reasonable agreement. The
measurement is of sufficient precision to allow refinements
in the understanding of the transverse momentum
distribution. © 2012 American Physical Society.},
Doi = {10.1103/PhysRevD.86.052010},
Key = {fds307811}
}
@article{fds321072,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdinov, O and Abeloos, B and Aben, R and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Affolder, AA and Agatonovic-Jovin, T and Agricola, J and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alstaty, M and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amako, K and Amaral
Coutinho, Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu,
LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos, N and Annovi, A and Antonelli, M and Antonov,
A and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai,
Y and Araque, JP and Arce, ATH and Arduh, FA and Arguin, JF and Argyropoulos, S and Arik, M and Armbruster, AJ and Armitage, LJ and Arnaez, O and Arnold, H and Arratia, M and Arslan, O and Artamonov,
A},
Title = {Transverse momentum, rapidity, and centrality dependence of
inclusive charged-particle production in sNN=5.02
TeV p + Pb collisions measured by the ATLAS
experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {763},
Pages = {313-336},
Publisher = {Elsevier BV},
Year = {2016},
Month = {December},
url = {http://dx.doi.org/10.1016/j.physletb.2016.10.053},
Abstract = {Measurements of the per-event charged-particle yield as a
function of the charged-particle transverse momentum and
rapidity are performed using p+Pb collision data collected
by the ATLAS experiment at the LHC at a centre-of-mass
energy of sNN=5.02TeV. Charged particles are reconstructed
over pseudorapidity |η|<2.3 and transverse momentum between
0.1 GeV and 22 GeV in a dataset corresponding to an
integrated luminosity of 1 μb−1. The results are
presented in the form of charged-particle nuclear
modification factors, where the p+Pb charged-particle
multiplicities are compared between central and peripheral
p+Pb collisions as well as to charged-particle cross
sections measured in pp collisions. The p+Pb collision
centrality is characterized by the total transverse energy
measured in −4.9<η<−3.1, which is in the direction of
the outgoing lead beam. Three different estimations of the
number of nucleons participating in the p+Pb collision are
carried out using the Glauber model and two Glauber–Gribov
colour-fluctuation extensions to the Glauber model. The
values of the nuclear modification factors are found to vary
significantly as a function of rapidity and transverse
momentum. A broad peak is observed for all centralities and
rapidities in the nuclear modification factors for
charged-particle transverse momentum values around 3 GeV.
The magnitude of the peak increases for more central
collisions as well as rapidity ranges closer to the
direction of the outgoing lead nucleus.},
Doi = {10.1016/j.physletb.2016.10.053},
Key = {fds321072}
}
@article{fds316849,
Author = {Aad, G and Abajyan, T and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim, AA and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya,
BS and Adamczyk, L and Adams, DL and Addy, TN and Adelman, J and Adomeit,
S and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Åkesson, TPA and Akimoto, G and Akimov, AV and Alam, MA and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allison, LJ and Allport, PP and Allwood-Spiers,
SE and Almond, J and Aloisio, A and Alon, R and Alonso, A and Alonso, F and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Ammosov, VV and Amor Dos
Santos and SP and Amorim, A and Amoroso, S and Amram, N and Anastopoulos,
C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei, V and Anduaga, XS and Angelidakis, S and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoki, M and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Argyropoulos, S and Arik,
E},
Title = {Triggers for displaced decays of long-lived neutral
particles in the ATLAS detector},
Journal = {Journal of Instrumentation},
Volume = {8},
Number = {7},
Pages = {P07015-P07015},
Publisher = {IOP Publishing},
Year = {2013},
Month = {January},
url = {http://dx.doi.org/10.1088/1748-0221/8/07/P07015},
Abstract = {A set of three dedicated triggers designed to detect
long-lived neutral particles decaying throughout the ATLAS
detector to a pair of hadronic jets is described. The
efficiencies of the triggers for selecting displaced decays
as a function of the decay position are presented for
simulated events. The effect of pile-up interactions on the
trigger efficiencies and the dependence of the trigger rate
on instantaneous luminosity during the 2012 data-taking
period at the LHC are discussed.},
Doi = {10.1088/1748-0221/8/07/P07015},
Key = {fds316849}
}
@article{fds332351,
Author = {Abazov, VM and Abbott, B and Abdesselam, A and Abolins, M and Abramov,
V and Acharya, BS and Adams, DL and Adams, M and Ahmed, SN and Alexeev, GD and Alton, A and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Arnoud, Y and Avila, C and Baarmand, MM and Babintsev, VV and Babukhadia, L and Bacon, TC and Baden, A and Balamurali, V and Baldin,
B and Balm, PW and Banerjee, S and Bantly, J and Barberis, E and Baringer,
P and Barreto, J and Bartlett, JF and Bassler, U and Bauer, D and Bean, A and Beaudette, F and Begel, M and Belyaev, A and Beri, SB and Bernardi, G and Bertram, I and Besson, A and Beuselinck, R and Bezzubov, VA and Bhat,
PC and Bhatnagar, V and Bhattacharjee, M and Blazey, G and Blekman, F and Blessing, S and Boehnlein, A and Bojko, NI and Bolton, TA and Borcherding, F and Bos, K and Bose, T and Brandt, A and Breedon, R and Briskin, G and Brock, R and Brooijmans, G and Bross, A and Buchholz, D and Buehler, M and Buescher, V and Burtovoi, VS and Butler, JM and Canelli,
F and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chan, KM and Chang, SM and Chekulaev, SV and Cho, DK and Choi, S and Chopra, S and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Coney, L and Connolly, B and Cooper, WE and Coppage, D and Crépé-Renaudin, S and Cretsinger, C and Cummings, MAC and Cutts, D and Davis, GA and De, K and de Jong, SJ and Demarteau, M and Demina, R and Demine, P and Denisov, D and Denisov,
SP},
Title = {tt̄ production cross section in pp̄ collisions at √s =
1.8 TeV},
Journal = {Physical Review D},
Volume = {67},
Number = {1},
Publisher = {American Physical Society (APS)},
Year = {2003},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.67.012004},
Abstract = {Results are presented on a measurement of the tt̄ pair
production cross section in pp̄ collisions at √s = 1.8
TeV from nine independent decay channels. The data were
collected by the DØ experiment during the 1992-1996 run of
the Fermilab Tevatron Collider. A total of 80 candidate
events is observed with an expected background of 38.8±3.3
events. For a top quark mass of 172.1 GeV/c2, the measured
cross section is 5.69 ±1.21(stat)±1.04(syst) pb. © 2003
The American Physical Society.},
Doi = {10.1103/PhysRevD.67.012004},
Key = {fds332351}
}
@article{fds346167,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdinov, O and Aben, R and Abi, B and Abolins, M and AbouZeid, OS and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adamczyk, L and Adams, DL and Adelman, J and Adomeit, S and Adye, T and Agatonovic-Jovin, T and Aguilar-Saavedra, JA and Agustoni, M and Ahlen, SP and Ahmadov, F and Aielli, G and Akerstedt, H and Åkesson,
TPA and Akimoto, G and Akimov, AV and Alberghi, GL and Albert, J and Albrand, S and Alconada Verzini and MJ and Aleksa, M and Aleksandrov,
IN and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Alimonti, G and Alio, L and Alison, J and Allbrooke, BMM and Allison, LJ and Allport, PP and Almond, J and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Altheimer, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amorim, A and Amoroso, S and Amram, N and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza,
A and Andrei, V and Anduaga, XS and Angelidakis, S and Angelozzi, I and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, AV and Anjos,
N and Annovi, A and Antonaki, A and Antonelli, M and Antonov, A and Antos,
J and Anulli, F and Aoki, M and Aperio Bella and L and Apolle, R and Arabidze,
G and Aracena, I and Arai, Y and Araque, JP and Arce, ATH and Arguin, J-F and Argyropoulos, S and Arik, M and Armbruster, AJ and Arnaez, O and Arnal,
V and Arnold, H and Arratia, M and Arslan, O and Artamonov, A and Artoni,
G and Asai, S and Asbah, N and Ashkenazi, A and Åsman, B and Asquith, L and Assamagan, K and Astalos, R and Atkinson, M and Atlay, NB and Auerbach,
B and Augsten, K and Aurousseau, M and Avolio, G and Azuelos, G and Azuma,
Y and Baak, MA and Baas, AE and Bacci, C and Bachacou, H and Bachas, K and Backes, M and Backhaus, M and Backus Mayes and J and Badescu, E and Bagiacchi, P and Bagnaia, P and Bai, Y and Bain, T and Baines, JT and Baker, OK and Balek, P and Balli, F and Banas, E and Banerjee, S and Bannoura, AAE and Bansal, V and Bansil, HS and Barak, L and Baranov, SP and Barberio, EL and Barberis, D and Barbero, M and Barillari, T and Barisonzi, M and Barklow, T and Barlow, N and Barnett, BM and Barnett,
RM and Barnovska, Z and Baroncelli, A and Barone, G and Barr, AJ and Barreiro, F and Barreiro Guimarães da Costa and J and Bartoldus, R and Barton, AE and Bartos, P and Bartsch, V and Bassalat, A and Basye, A and Bates, RL and Batley, JR and Battaglia, M and Battistin, M and Bauer, F and Bawa, HS and Beattie, MD and Beau, T and Beauchemin, PH and Beccherle,
R and Bechtle, P and Beck, HP and Becker, K and Becker, S and Beckingham,
M and Becot, C and Beddall, AJ and Beddall, A and Bedikian, S and Bednyakov, VA and Bee, CP and Beemster, LJ and Beermann, TA and Begel,
M and Behr, JK and Belanger-Champagne, C and Bell, PJ and Bell, WH and Bella, G and Bellagamba, L and Bellerive, A and Bellomo, M and Belotskiy, K and Beltramello, O and Benary, O and Benchekroun, D and Bendtz, K and Benekos, N and Benhammou, Y and Benhar Noccioli and E and Benitez Garcia and JA and Benjamin, DP and Bensinger, JR and Benslama,
K and Bentvelsen, S and Berge, D and Bergeaas Kuutmann and E and Berger, N and Berghaus, F and Beringer, J and Bernard, C and Bernat, P and Bernius, C and Bernlochner, FU and Berry, T and Berta, P and Bertella, C and Bertoli,
G and Bertolucci, F and Bertsche, C and Bertsche, D and Besana, MI and Besjes, GJ and Bessidskaia Bylund and O and Bessner, M and Besson, N and Betancourt, C and Bethke, S and Bhimji, W and Bianchi, RM and Bianchini,
L and Bianco, M and Biebel, O and Bieniek, SP and Bierwagen, K and Biesiada, J and Biglietti, M and Bilbao De Mendizabal and J and Bilokon,
H and Bindi, M and Binet, S and Bingul, A and Bini, C and Black, CW and Black,
JE and Black, KM and Blackburn, D and Blair, RE and Blanchard, J-B and Blazek, T and Bloch, I and Blocker, C and Blum, W and Blumenschein, U and Bobbink, GJ and Bobrovnikov, VS and Bocchetta, SS and Bocci, A and Bock,
C and Boddy, CR and Boehler, M and Boek, TT and Bogaerts, JA and Bogdanchikov, AG and Bogouch, A and Bohm, C and Bohm, J and Boisvert, V and Bold, T and Boldea, V and Boldyrev, AS and Bomben, M and Bona, M and Boonekamp, M and Borisov, A and Borissov, G and Borri, M and Borroni, S and Bortfeldt, J and Bortolotto, V and Bos, K and Boscherini, D and Bosman,
M and Boterenbrood, H and Boudreau, J and Bouffard, J and Bouhova-Thacker, EV and Boumediene, D and Bourdarios, C and Bousson,
N and Boutouil, S and Boveia, A and Boyd, J and Boyko, IR and Bozic, I and Bracinik, J and Brandt, A and Brandt, G and Brandt, O and Bratzler, U and Brau, B and Brau, JE and Braun, HM and Brazzale, SF and Brelier, B and Brendlinger, K and Brennan, AJ and Brenner, R and Bressler, S and Bristow, K and Bristow, TM and Britton, D and Brochu, FM and Brock, I and Brock, R and Bromberg, C and Bronner, J and Brooijmans, G and Brooks, T and Brooks, WK and Brosamer, J and Brost, E and Brown, J and Bruckman de
Renstrom, PA and Bruncko, D and Bruneliere, R and Brunet, S and Bruni,
A and Bruni, G and Bruschi, M and Bryngemark, L and Buanes, T and Buat, Q and Bucci, F and Buchholz, P and Buckingham, RM and Buckley, AG and Buda,
SI and Budagov, IA and Buehrer, F and Bugge, L and Bugge, MK and Bulekov,
O and Bundock, AC and Burckhart, H and Burdin, S and Burghgrave, B and Burke, S and Burmeister, I and Busato, E and Büscher, D and Büscher,
V and Bussey, P and Buszello, CP and Butler, B and Butler, JM and Butt, AI and Buttar, CM and Butterworth, JM and Butti, P and Buttinger, W and Buzatu,
A and Byszewski, M and Cabrera Urbán and S and Caforio, D and Cakir, O and Calafiura, P and Calandri, A and Calderini, G and Calfayan, P and Calkins, R and Caloba, LP and Calvet, D and Calvet, S and Camacho Toro,
R and Camarda, S and Cameron, D and Caminada, LM and Caminal Armadans,
R and Campana, S and Campanelli, M and Campoverde, A and Canale, V and Canepa, A and Cano Bret and M and Cantero, J and Cantrill, R and Cao, T and Capeans Garrido and MDM and Caprini, I and Caprini, M and Capua, M and Caputo, R and Cardarelli, R and Carli, T and Carlino, G and Carminati,
L and Caron, S and Carquin, E and Carrillo-Montoya, GD and Carter, JR and Carvalho, J and Casadei, D and Casado, MP and Casolino, M and Castaneda-Miranda, E and Castelli, A and Castillo Gimenez and V and Castro, NF and Catastini, P and Catinaccio, A and Catmore, JR and Cattai, A and Cattani, G and Caudron, J and Cavaliere, V and Cavalli, D and Cavalli-Sforza, M and Cavasinni, V and Ceradini, F and Cerio, BC and Cerny, K and Cerqueira, AS and Cerri, A and Cerrito, L and Cerutti, F and Cerv, M and Cervelli, A and Cetin, SA and Chafaq, A and Chakraborty, D and Chalupkova, I and Chang, P and Chapleau, B and Chapman, JD and Charfeddine, D and Charlton, DG and Chau, CC and Chavez Barajas and CA and Cheatham, S and Chegwidden, A and Chekanov, S and Chekulaev, SV and Chelkov, GA and Chelstowska, MA and Chen, C and Chen, H and Chen, K and Chen, L and Chen, S and Chen, X and Chen, Y and Cheng, HC and Cheng, Y and Cheplakov, A and Cherkaoui El Moursli and R and Chernyatin, V and Cheu,
E and Chevalier, L and Chiarella, V and Chiefari, G and Childers, JT and Chilingarov, A and Chiodini, G and Chisholm, AS and Chislett, RT and Chitan, A and Chizhov, MV and Chouridou, S and Chow, BKB and Chromek-Burckhart, D and Chu, ML and Chudoba, J and Chwastowski, JJ and Chytka, L and Ciapetti, G and Ciftci, AK and Ciftci, R and Cinca, D and Cindro, V and Ciocio, A and Cirkovic, P and Citron, ZH and Ciubancan, M and Clark, A and Clark, PJ and Clarke, RN and Cleland, W and Clemens, JC and Clement, C and Coadou, Y and Cobal, M and Coccaro, A and Cochran, J and Coffey, L},
Title = {Two-particle Bose-Einstein correlations in pp
collisions at [Formula: see text] 0.9 and 7 TeV measured
with the ATLAS detector.},
Journal = {The European physical journal. C, Particles and
fields},
Volume = {75},
Number = {10},
Pages = {466},
Year = {2015},
Month = {January},
url = {http://dx.doi.org/10.1140/epjc/s10052-015-3644-x},
Abstract = {The paper presents studies of Bose-Einstein Correlations
(BEC) for pairs of like-sign charged particles measured in
the kinematic range [Formula: see text] 100 MeV and
[Formula: see text] 2.5 in proton collisions at
centre-of-mass energies of 0.9 and 7 TeV with the ATLAS
detector at the CERN Large Hadron Collider. The integrated
luminosities are approximately 7 [Formula: see
text]b[Formula: see text], 190 [Formula: see
text]b[Formula: see text] and 12.4 nb[Formula: see text]
for 0.9 TeV, 7 TeV minimum-bias and 7 TeV
high-multiplicity data samples, respectively. The
multiplicity dependence of the BEC parameters characterizing
the correlation strength and the correlation source size are
investigated for charged-particle multiplicities of up to
240. A saturation effect in the multiplicity dependence of
the correlation source size parameter is observed using the
high-multiplicity 7 TeV data sample. The dependence of the
BEC parameters on the average transverse momentum of the
particle pair is also investigated.},
Doi = {10.1140/epjc/s10052-015-3644-x},
Key = {fds346167}
}
@article{fds364958,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Khoury, KA and Alberghi,
GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen,
BW and Allport, PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez Estevez and M and Álvarez
Piqueras, D and Alviggi, MG and Amaral Coutinho and Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders, JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony, MT and Antonelli, M and Antrim, DJA and Anulli, F and Aoki, M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque, JP and Araujo Ferraz and V and Araujo Pereira,
R},
Title = {Two-particle Bose–Einstein correlations in pp collisions
at √s=13 TeV measured with the ATLAS detector at the
LHC},
Journal = {European Physical Journal C},
Volume = {82},
Number = {7},
Year = {2022},
Month = {July},
url = {http://dx.doi.org/10.1140/epjc/s10052-022-10472-0},
Abstract = {This paper presents studies of Bose–Einstein correlations
(BEC) in proton–proton collisions at a centre-of-mass
energy of 13 TeV, using data from the ATLAS detector at the
CERN Large Hadron Collider. Data were collected in a special
low-luminosity configuration with a minimum-bias trigger and
a high-multiplicity track trigger, accumulating integrated
luminosities of 151 μ b- 1 and 8.4 nb- 1, respectively.
The BEC are measured for pairs of like-sign charged
particles, each with | η| < 2.5 , for two kinematic ranges:
the first with particle pT> 100 MeV and the second with
particle pT> 500 MeV. The BEC parameters, characterizing the
source radius and particle correlation strength, are
investigated as functions of charged-particle multiplicity
(up to 300) and average transverse momentum of the pair (up
to 1.5 GeV). The double-differential dependence on
charged-particle multiplicity and average transverse
momentum of the pair is also studied. The BEC radius is
found to be independent of the charged-particle multiplicity
for high charged-particle multiplicity (above 100),
confirming a previous observation at lower energy. This
saturation occurs independent of the transverse momentum of
the pair.},
Doi = {10.1140/epjc/s10052-022-10472-0},
Key = {fds364958}
}
@article{fds307797,
Author = {Aad, G and Abbott, B and Abdallah, J and Abdel Khalek and S and Abdelalim,
AA and Abdinov, O and Abi, B and Abolins, M and Abouzeid, OS and Abramowicz, H and Abreu, H and Acerbi, E and Acharya, BS and Adamczyk,
L and Adams, DL and Addy, TN and Adelman, J and Adomeit, S and Adragna, P and Adye, T and Aefsky, S and Aguilar-Saavedra, JA and Aharrouche, M and Ahlen, SP and Ahles, F and Ahmad, A and Ahsan, M and Aielli, G and Akdogan,
T and Akesson, TPA and Akimoto, G and Akimov, AV and Akiyama, A and Alam,
MS and Alam, MA and Albert, J and Albrand, S and Aleksa, M and Aleksandrov,
IN and Alessandria, F and Alexa, C and Alexander, G and Alexandre, G and Alexopoulos, T and Alhroob, M and Aliev, M and Alimonti, G and Alison,
J and Allbrooke, BMM and Allport, PP and Allwood-Spiers, SE and Almond,
J and Aloisio, A and Alon, R and Alonso, A and Alvarez Gonzalez and B and Alviggi, MG and Amako, K and Amelung, C and Ammosov, VV and Amorim, A and Amram, N and Anastopoulos, C and Ancu, LS and Andari, N and Andeen, T and Anders, CF and Anders, G and Anderson, KJ and Andreazza, A and Andrei,
V and Anduaga, XS and Anger, P and Angerami, A and Anghinolfi, F and Anisenkov, A and Anjos, N and Annovi, A and Antonaki, A and Antonelli,
M and Antonov, A and Antos, J and Anulli, F and Aoun, S and Aperio Bella,
L and Apolle, R and Arabidze, G and Aracena, I and Arai, Y and Arce, ATH and Arfaoui, S and Arguin, JF and Arik, E and Arik, M and Armbruster, AJ and Arnaez, O and Arnal, V and Arnault, C and Artamonov, A and Artoni,
G},
Title = {Underlying event characteristics and their dependence on jet
size of charged-particle jet events in pp collisions at
√(s)=7TeV with the ATLAS detector},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {86},
Number = {7},
Publisher = {American Physical Society (APS)},
Year = {2012},
Month = {October},
url = {http://dx.doi.org/10.1103/PhysRevD.86.072004},
Abstract = {Distributions sensitive to the underlying event are studied
in events containing one or more charged-particle jets
produced in pp collisions at √s=7TeV with the ATLAS
detector at the Large Hadron Collider (LHC). These
measurements reflect 800μb-1 of data taken during 2010.
Jets are reconstructed using the anti-kt algorithm with
radius parameter R varying between 0.2 and 1.0.
Distributions of the charged-particle multiplicity, the
scalar sum of the transverse momentum of charged particles,
and the average charged-particle pT are measured as
functions of pTjet in regions transverse to and opposite the
leading jet for 4GeV<pTjet<100GeV. In addition, the R
dependence of the mean values of these observables is
studied. In the transverse region, both the multiplicity and
the scalar sum of the transverse momentum at fixed pTjet
vary significantly with R, while the average
charged-particle transverse momentum has a minimal
dependence on R. Predictions from several Monte Carlo tunes
have been compared to the data; the predictions from Pythia
6, based on tunes that have been determined using LHC data,
show reasonable agreement with the data, including the
dependence on R. Comparisons with other generators indicate
that additional tuning of soft-QCD parameters is necessary
for these generators. The measurements presented here
provide a testing ground for further development of the
Monte Carlo models. © 2012 CERN.},
Doi = {10.1103/PhysRevD.86.072004},
Key = {fds307797}
}
@article{fds346202,
Author = {Naga Prasad and SV and Duan, Z-H and Gupta, MK and Surampudi, VSK and Volinia, S and Calin, GA and Liu, C-G and Kotwal, A and Moravec, CS and Starling, RC and Perez, DM and Sen, S and Wu, Q and Plow, EF and Croce, CM and Karnik, S},
Title = {Unique microRNA profile in end-stage heart failure indicates
alterations in specific cardiovascular signaling
networks.},
Journal = {The Journal of biological chemistry},
Volume = {284},
Number = {40},
Pages = {27487-27499},
Year = {2009},
Month = {October},
url = {http://dx.doi.org/10.1074/jbc.m109.036541},
Abstract = {It is well established that gene expression patterns are
substantially altered in cardiac hypertrophy and heart
failure, but the reasons for such differences are not clear.
MicroRNAs (miRNAs) are short noncoding RNAs that provide a
novel mechanism for gene regulation. The goal of this study
was to comprehensively test for alterations in miRNA
expression using human heart failure samples with an aim to
build signaling pathway networks using predicted targets for
the miRNAs and to identify nodal molecules that control
these networks. Genome-wide profiling of miRNAs was
performed using custom-designed miRNA microarray followed by
validation on an independent set of samples. Eight miRNAs
are significantly altered in heart failure of which we have
identified two novel miRNAs that are yet to be implicated in
cardiac pathophysiology. To gain an unbiased global
perspective on regulation by altered miRNAs, predicted
targets of eight miRNAs were analyzed using the Ingenuity
Pathways Analysis network algorithm to build signaling
networks and identify nodal molecules. The majority of nodal
molecules identified in our analysis are targets of altered
miRNAs and are known regulators of cardiovascular signaling.
A heart failure gene expression data base was used to
analyze changes in expression patterns for these target
nodal molecules. Indeed, expression of nodal molecules was
altered in heart failure and inversely correlated to miRNA
changes validating our analysis. Importantly, using network
analysis we have identified a limited number of key
functional targets that may regulate expression of the
myriad proteins in heart failure and could be potential
therapeutic targets.},
Doi = {10.1074/jbc.m109.036541},
Key = {fds346202}
}
@article{fds346207,
Author = {Prakash, J and Singh, PK and Kotwal, A and Ramakrishnan,
TS},
Title = {Unknown Poisoning Amongst Serving Personnel.},
Journal = {Medical journal, Armed Forces India},
Volume = {65},
Number = {1},
Pages = {41-43},
Year = {2009},
Month = {January},
url = {http://dx.doi.org/10.1016/s0377-1237(09)80053-1},
Abstract = {<h4>Background</h4>Poisoning is recognized as an important
health problem in many countries of the world. There is
incomplete information on poisoning accidents, which is a
major problem in developing countries.<h4>Methods</h4>A
cross-sectional analysis of hospital records of armed forces
personnel admitted with a provisional diagnosis of unknown
poisoning was carried out.<h4>Result</h4>Unknown poisoning
represented 0.25% of hospital admissions and 6584 man-hours
were lost. 85% poisonings occurred at railway station and
majority were food related. Average length of stay in the
hospital was 14.69 days. Ten patients required intensive
care and two patients were admitted to the psychiatry
ward.<h4>Conclusion</h4>Majority of the incidents occurred
in railways, signifying the importance of health education
and precaution while proceeding on leave. Since, most of the
affected were young soldiers, education should start from
recruiting centers. Few patients had alcohol intoxication
reflecting their dependence potential and need for
reinforcing prohibition on alcohol consumption during
travel.},
Doi = {10.1016/s0377-1237(09)80053-1},
Key = {fds346207}
}
@article{fds307933,
Author = {Aaltonen, and T, and others},
Title = {Updated search for the flavor-changing neutral-current decay
$D^{0}\rightarrow{}\mu{}^{+}\mu{}^{-}$ in $pp[over
\ifmmode\bar\else\textasciimacron\fi{}]$ collisions at
$\sqrt{s}=1.96$ TeV},
Journal = {Phys. Rev. D},
Volume = {82},
Number = {9},
Pages = {091105},
Publisher = {American Physical Society},
Year = {2010},
Month = {November},
url = {http://dx.doi.org/10.1103/PhysRevD.82.091105},
Abstract = {We report on a search for the flavor-changing
neutral-current decay D0→μ⊃+μ⊃- in pp̄ collisions
at √s=1.96TeV using 360pb⊃-1 of integrated luminosity
collected by the CDF II detector at the Fermilab Tevatron
collider. A displaced vertex trigger selects long-lived D0
candidates in the μ⊃+μ⊃-, π⊃+π⊃-, and
K⊃-π⊃+ decay modes. We use the Cabibbo-favored
D0→K⊃- π⊃+ channel to optimize the selection criteria
in an unbiased manner, and the kinematically similar
D0→π⊃+π⊃- channel for normalization. We set an upper
limit on the branching fraction B(D0→μ⊃+μ⊃-)<2.1×10⊃-7(3.0×10⊃-7)
at the 90% (95%) confidence level. © 2010 The American
Physical Society.},
Doi = {10.1103/PhysRevD.82.091105},
Key = {fds307933}
}
@article{fds307634,
Author = {Aaltonen, T and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel, JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar,
F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd,
HS and Burkett, K and Busetto, G and Bussey, P and Butti, P and Buzatu, A and Calamba, A and Camarda, S and Campanelli, M and Canelli, F and Carls, B and Carlsmith, D and Carosi, R and Carrillo, S and Casal, B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere, V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok,
M and Chiarelli, G and Chlachidze, G and Cho, K and Chokheli, D and Ciocci,
MA and Clark, A and Clarke, C and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Cremonesi, M and Cruz, D and Cuevas, J and Culbertson, R and D'Ascenzo, N and Datta, M and De
Barbaro, P and Demortier, L and Deninno, M and Devoto, F and D'Errico,
M and Di Canto and A and Di Ruzza and B and Dittmann, JR and D'Onofrio, M and Donati, S and Dorigo, M and Driutti, A and Ebina, K and Edgar, R and Elagin, A},
Title = {Updated search for the standard model Higgs boson in events
with jets and missing transverse energy using the full CDF
data set},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {87},
Number = {5},
Publisher = {American Physical Society (APS)},
Year = {2013},
Month = {March},
url = {http://dx.doi.org/10.1103/PhysRevD.87.052008},
Abstract = {We present an updated search for the Higgs boson produced in
association with a vector boson in the final state with
missing transverse energy and two jets. We use the full CDF
data set corresponding to an integrated luminosity of 9.45
fb-1 at a proton-antiproton center-of-mass energy of
√s=1.96 TeV. New to this analysis is the inclusion of a
b-jet identification algorithm specifically optimized for
H→bb̄ searches. Across the Higgs boson mass range
90≤mH≤150 GeV/c2, the expected 95% credibility level
upper limits on the VH production cross section times the
H→bb̄ branching fraction are improved by an average of
14% relative to the previous analysis. At a Higgs boson mass
of 125 GeV/c2, the observed (expected) limit is 3.06 (3.33)
times the standard model prediction, corresponding to one of
the most sensitive searches to date in this final state. ©
2013 American Physical Society.},
Doi = {10.1103/PhysRevD.87.052008},
Key = {fds307634}
}
@article{fds364961,
Author = {Buarque Franzosi and D and Gallinaro, M and Ruiz, R and Aarrestad, TK and Cetorelli, F and Chiesa, M and Costantini, A and Denner, A and Dittmaier, S and Franken, R and Govoni, P and Han, T and Kotwal, AV and Li,
J and Lohwasser, K and Long, K and Ma, Y and Mantani, L and Marchegiani, M and Pellen, M and Pelliccioli, G and Potamianos, K and Reuter, J and Schmidt, T and Schwan, C and Szleper, M and Verheyen, R and Xie, K and Zhang, R},
Title = {Vector boson scattering processes: Status and
prospects},
Journal = {Reviews in Physics},
Volume = {8},
Year = {2022},
Month = {June},
url = {http://dx.doi.org/10.1016/j.revip.2022.100071},
Abstract = {Insight into the electroweak (EW) and Higgs sectors can be
achieved through measurements of vector boson scattering
(VBS) processes. The scattering of EW bosons are rare
processes that are precisely predicted in the Standard Model
(SM) and are closely related to the Higgs mechanism.
Modifications to VBS processes are also predicted in models
of physics beyond the SM (BSM), for example through changes
to the Higgs boson couplings to gauge bosons and the
resonant production of new particles. In this review,
experimental results and theoretical developments of VBS at
the Large Hadron Collider, its high luminosity upgrade, and
future colliders are presented.},
Doi = {10.1016/j.revip.2022.100071},
Key = {fds364961}
}
@article{fds340914,
Author = {Thurman Keup and RM and Kotwal, AV and Tecchio, M and Byon Wagner,
A},
Title = {W boson physics at hadron colliders},
Journal = {Reviews of Modern Physics},
Volume = {73},
Number = {267},
Pages = {40},
Year = {2001},
Month = {April},
Abstract = {The use of hadron colliders to investigate the properties of
the W bosons started in 1982 at the CERN SpS collider. Since
then, the Tevatron experiments at Fermilab have recorded a
large sample of W events which allowed precision
measurements of the properties of W bosons. In this paper
the authors review W gauge boson physics at hadron colliders
from 1982 to 2000. They first discuss the production
mechanism and detection of W bosons in p collisions. After a
brief review of the early studies, W boson physics at the
Tevatron collider are thoroughly examined. Finally, possible
future directions of W boson physics at hadron colliders are
discussed.},
Key = {fds340914}
}
@article{fds308193,
Author = {Thurman-Keup, RM and Kotwal, AV and Tecchio, M and Byon-Wagner,
A},
Title = {W boson physics at hadron colliders},
Journal = {Reviews of Modern Physics},
Volume = {73},
Number = {2},
Pages = {267-306},
Publisher = {American Physical Society (APS)},
Year = {2001},
Month = {April},
url = {http://dx.doi.org/10.1103/RevModPhys.73.267},
Abstract = {The use of hadron colliders to investigate the properties of
the W bosons started in 1982 at the CERN Spp̄S collider.
Since then, the Tevatron experiments at Fermilab have
recorded a large sample of W events which allowed precision
measurements of the properties of W bosons. In this paper
the authors review W gauge boson physics at hadron colliders
from 1982 to 2000. They first discuss the production
mechanism and detection of W bosons in pp̄ collisions.
After a brief review of the early studies, W boson physics
at the Tevatron collider are thoroughly examined. Finally,
possible future directions of W boson physics at hadron
colliders are discussed.},
Doi = {10.1103/RevModPhys.73.267},
Key = {fds308193}
}
@article{fds331625,
Author = {Aaltonen, T and Álvarez González, B and Amerio, S and Amidei, D and Anastassov, A and Annovi, A and Antos, J and Apollinari, G and Appel,
JA and Arisawa, T and Artikov, A and Asaadi, J and Ashmanskas, W and Auerbach, B and Aurisano, A and Azfar, F and Badgett, W and Bae, T and Barbaro-Galtieri, A and Barnes, VE and Barnett, BA and Barria, P and Bartos, P and Bauce, M and Bedeschi, F and Behari, S and Bellettini, G and Bellinger, J and Benjamin, D and Beretvas, A and Bhatti, A and Bisello,
D and Bizjak, I and Bland, KR and Blumenfeld, B and Bocci, A and Bodek, A and Bortoletto, D and Boudreau, J and Boveia, A and Brigliadori, L and Bromberg, C and Brucken, E and Budagov, J and Budd, HS and Burkett, K and Busetto, G and Bussey, P and Buzatu, A and Calamba, A and Calancha, C and Camarda, S and Campanelli, M and Campbell, M and Canelli, F and Carls,
B and Carlsmith, D and Carosi, R and Carrillo, S and Carron, S and Casal,
B and Casarsa, M and Castro, A and Catastini, P and Cauz, D and Cavaliere,
V and Cavalli-Sforza, M and Cerri, A and Cerrito, L and Chen, YC and Chertok, M and Chiarelli, G and Chlachidze, G and Chlebana, F and Cho,
K and Chokheli, D and Chung, WH and Chung, YS and Ciocci, MA and Clark, A and Clarke, C and Compostella, G and Convery, ME and Conway, J and Corbo, M and Cordelli, M and Cox, CA and Cox, DJ and Crescioli, F and Cuevas, J and Culbertson, R and Dagenhart, D and D'Ascenzo, N and Datta, M and De
Barbaro, P and Dell'Orso, M and Demortier, L and Deninno, M and Devoto,
F and D'Errico, M},
Title = {W-boson polarization measurement in the tt- dilepton channel
using the CDF II detector},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {722},
Number = {1-3},
Pages = {48-54},
Publisher = {Elsevier BV},
Year = {2013},
Month = {May},
url = {http://dx.doi.org/10.1016/j.physletb.2013.03.032},
Abstract = {We present a measurement of the W-boson polarization in
top-quark decays in tt- events with decays to dilepton final
states using data corresponding to 5.1 fb-1 of integrated
luminosity in pp- collisions collected by the CDF II
detector at the Tevatron. Assuming a top-quark mass of 172.5
GeV/c2, a simultaneous measurement of the fractions of
longitudinal ( f0) and right-handed ( f+) W-bosons yields
the results f0 = 0.70-0.17+0.18 (stat) ± 0.06(syst) and f+
=-0.09 ± 0.09(stat) ± 0.03(syst). Combining this
measurement with our previous measurement based on
single-lepton final states, we obtain f0 = 0.84 ±
0.09(stat) ± 0.05(syst) and f+ =-0.16 ± 0.05(stat) ±
0.04(syst). The results are consistent with the standard
model expectation.},
Doi = {10.1016/j.physletb.2013.03.032},
Key = {fds331625}
}
@article{fds356537,
Author = {Aad, G and Abbott, B and Abbott, DC and Abed Abud and A and Abeling, K and Abhayasinghe, DK and Abidi, SH and AbouZeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abulaiti, Y and Acharya, BS and Achkar,
B and Adachi, S and Adam, L and Adam Bourdarios and C and Adamczyk, L and Adamek, L and Adelman, J and Adersberger, M and Adiguzel, A and Adorni,
S and Adye, T and Affolder, AA and Afik, Y and Agapopoulou, C and Agaras,
MN and Aggarwal, A and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahmadov, F and Ahmed, WS and Ai, X and Aielli, G and Akatsuka, S and Åkesson, TPA and Akilli, E and Akimov, AV and Al Khoury and K and Alberghi, GL and Albert, J and Alconada Verzini and MJ and Alderweireldt, S and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexandre, D and Alexopoulos, T and Alfonsi, A and Alfonsi, F and Alhroob, M and Ali, B and Alimonti, G and Alison, J and Alkire, SP and Allaire, C and Allbrooke, BMM and Allen, BW and Allport, PP and Aloisio,
A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alvarez
Estevez, M and Álvarez Piqueras, D and Alviggi, MG and Amaral
Coutinho, Y and Ambler, A and Ambroz, L and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amrouche, CS and An, F and Anastopoulos, C and Andari, N and Andeen, T and Anders, CF and Anders,
JK and Andreazza, A and Andrei, V and Anelli, CR and Angelidakis, S and Angerami, A and Anisenkov, AV and Annovi, A and Antel, C and Anthony,
MT and Antipov, E and Antonelli, M and Antrim, DJA and Anulli, F and Aoki,
M and Aparisi Pozo and JA and Aperio Bella and L and Arabidze, G and Araque,
JP},
Title = {Z boson production in Pb+Pb collisions at √Snn
= 5.02 TeV measured by the ATLAS experiment},
Journal = {Physics Letters, Section B: Nuclear, Elementary Particle and
High-Energy Physics},
Volume = {802},
Year = {2020},
Month = {March},
url = {http://dx.doi.org/10.1016/j.physletb.2020.135262},
Abstract = {The production yield of Z bosons is measured in the electron
and muon decay channels in Pb+Pb collisions at √Snn = 5.02
TeV with the ATLAS detector. Data from the 2015 LHC run
corresponding to an integrated luminosity of 0.49 nb-1 are
used for the analysis. The Z boson yield, normalised by the
total number of minimum-bias events and the mean nuclear
thickness function, is measured as a function of dilepton
rapidity and event centrality. The measurements in Pb+Pb
collisions are compared with similar measurements made in
proton-proton collisions at the same centre-of-mass energy.
The nuclear modification factor is found to be consistent
with unity for all centrality intervals. The results are
compared with theoretical predictions obtained at
next-to-leading order using nucleon and nuclear parton
distribution functions. The normalised Z boson yields in
Pb+Pb collisions lie 1-3σ above the predictions. The
nuclear modification factor measured as a function of
rapidity agrees with unity and is consistent with a
next-to-leading-order QCD calculation including the isospin
effect.},
Doi = {10.1016/j.physletb.2020.135262},
Key = {fds356537}
}
@article{fds356705,
Author = {Aaboud, M and Aad, G and Abbott, B and Abdinov, O and Abeloos, B and Abidi,
SH and Abouzeid, OS and Abraham, NL and Abramowicz, H and Abreu, H and Abreu, R and Abulaiti, Y and Acharya, BS and Adachi, S and AdamczyK, L and Adelman, J and Adersberger, M and Adye, T and Affolder, AA and AfiK, Y and Agatonovic-Jovin, T and Agheorghiesei, C and Aguilar-Saavedra, JA and Ahlen, SP and Ahmadov, F and Aielli, G and Akatsuka, S and Akerstedt, H and Åkesson, TPA and Akilli, E and Akimov, AV and Alberghi, GL and Albert,
J and Albicocco, P and Alconada Verzini and MJ and Alderweireldt, SC and Aleksa, M and Aleksandrov, IN and Alexa, C and Alexander, G and Alexopoulos, T and Alhroob, M and Ali, B and Aliev, M and Alimonti, G and Alison, J and Alkire, SP and Allbrooke, BMM and Allen, BW and Allport,
PP and Aloisio, A and Alonso, A and Alonso, F and Alpigiani, C and Alshehri, AA and Alstaty, MI and Alvarez Gonzalez and B and Álvarez
Piqueras, D and Alviggi, MG and Amadio, BT and Amaral Coutinho and Y and Amelung, C and Amidei, D and Amor Dos Santos and SP and Amoroso, S and Amundsen, G and Anastopoulos, C and Ancu, LS and Andari, N and Andeen,
T and Anders, CF and Anders, JK and Anderson, KJ and Andreazza, A and Andrei, V and Angelidakis, S and Angelozzi, I and Angerami, A and Anisenkov, AV and Anjos, N and Annovi, A and Antel, C and Antonelli, M and Antonov, A and Antrim, DJ and Anulli, F and Aoki, M and Aperio Bella and L and Arabidze, G and Arai, Y and Araque, JP and Araujo Ferraz and V and Arce,
ATH and Ardell, RE and Arduh, FA and Arguin, JF and Argyropoulos, S and AriK, M and Armbruster, AJ and Armitage, LJ},
Title = {Z Z → + - ′ + ′ - s-section measurements and search
for anomalous triple gauge couplings in 13 TeV p p
collisions with the ATLAS detector},
Journal = {Physical Review D},
Volume = {97},
Number = {3},
Year = {2018},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.97.032005},
Abstract = {Measurements of ZZ production in the +-′+′- channel in
proton-proton collisions at 13 TeV center-of-mass energy at
the Large Hadron Collider are presented. The data correspond
to 36.1 fb-1 of collisions collected by the ATLAS experiment
in 2015 and 2016. Here and ′ stand for electrons or muons.
Integrated and differential ZZ→+-′+′- cross sections
with Z→+- candidate masses in the range of 66 GeV to 116
GeV are measured in a fiducial phase space corresponding to
the detector acceptance and corrected for detector effects.
The differential cross sections are presented in bins of
twenty observables, including several that describe the jet
activity. The integrated cross section is also extrapolated
to a total phase space and to all standard model decays of Z
bosons with mass between 66 GeV and 116 GeV, resulting in a
value of 17.3±0.9[±0.6(stat)±0.5(syst)±0.6(lumi)] pb.
The measurements are found to be in good agreement with the
standard model. A search for neutral triple gauge couplings
is performed using the transverse momentum distribution of
the leading Z boson candidate. No evidence for such
couplings is found and exclusion limits are set on their
parameters.},
Doi = {10.1103/PhysRevD.97.032005},
Key = {fds356705}
}
@booklet{Abbott98k,
Author = {Abbott, B and Abolins, M and Acharya, BS and Adam, I and Adams, DL and Adams, M and Ahn, S and Aihara, H and Alves, GA and Amidi, E and Amos, N and Anderson, EW and Astur, R and Baarmand, MM and Baden, A and Balamurali,
V and Balderston, J and Baldin, B and Banerjee, S and Bantly, J and Barberis, E and Bartlett, JF and Bazizi, K and Belyaev, A and Beri, SB and Bertram, I and Bezzubov, VA and Bhat, PC and Bhatnagar, V and Bhattacharjee, M and Biswas, N and Blazey, G and Blessing, S and Bloom,
P and Boehnlein, A and Bojko, NI and Borcherding, F and Boswell, C and Brandt, A and Brock, R and Bross, A and Buchholz, D and Burtovoi, VS and Butler, JM and Carvalho, W and Casey, D and Casilum, Z and Castilla-Valdez, H and Chakraborty, D and Chang, SM and Chekulaev,
SV and Chen, LP and Chen, W and Choi, S and Chopra, S and Choudhary, BC and Christenson, JH and Chung, M and Claes, D and Clark, AR and Cobau, WG and Cochran, J and Cooper, WE and Cretsinger, C and Cullen-Vidal, D and Cummings, MAC and Cutts, D and Dahl, OI and Davis, K and De, K and Del
Signore, K and Demarteau, M and Denisov, D and Denisov, SP and Diehl,
HT and Diesburg, M and Di Loreto and G and Draper, P and Ducros, Y and Dudko,
LV and Dugad, SR and Edmunds, D and Ellison, J and Elvira, VD and Engelmann, R and Eno, S and Eppley, G and Ermolov, P and Eroshin, OV and Evdokimov, VN and Fahland, T and Fatyga, M and Fatyga, MK and Feher, S and Fein, D and Ferbel, T and Finocchiaro, G and Fisk, HE and Fisyak, Y and Flattum, E},
Title = {[Formula presented] production in [Formula presented]
collisions at [Formula presented] and limits on anomalous
[Formula presented] and [Formula presented]
couplings},
Journal = {Physical Review D - Particles, Fields, Gravitation and
Cosmology},
Volume = {57},
Number = {7},
Pages = {R3817-R3821},
Publisher = {American Physical Society (APS)},
Year = {1998},
Month = {January},
url = {http://dx.doi.org/10.1103/PhysRevD.57.R3817},
Abstract = {We present a study of (Formula presented) production in
(Formula presented) collisions at (Formula presented) from
97 (Formula presented) of data collected in the (Formula
presented) (μμγ) decay channel with the D0 detector at
Fermilab. The event yield and kinematic characteristics are
consistent with the standard model predictions. We obtain
limits on anomalous (Formula presented) and (Formula
presented) couplings for form factor scales (Formula
presented) and (Formula presented) Combining this analysis
with our previous results yields 95% C.L. limits (Formula
presented) (Formula presented) (Formula presented) and
(Formula presented) for a form factor scale (Formula
presented). © 1998 The American Physical
Society.},
Doi = {10.1103/PhysRevD.57.R3817},
Key = {Abbott98k}
}
@article{fds308021,
Author = {al, TAE},
Title = {``Direct measurement of the $W$ boson width in $p\overline
p$ Collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review Letters},
Volume = {85},
Number = {7},
Pages = {3347},
Year = {2000},
url = {http://dx.doi.org/10.1103/physrevlett.100.071801},
Abstract = {A direct measurement of the total decay width of the W boson
Gamma(W) is presented using 350 pb(-1) of data from pp[over
] collisions at square root s = 1.96 TeV collected with the
CDF II detector at the Fermilab Tevatron. The width is
determined by normalizing predicted signal and background
distributions to 230 185 W candidates decaying to enu and
micronu in the transverse-mass region 50<M(T)<90 GeV and
then fitting the predicted shape to 6055 events in the
high-M(T) region, 90<M(T)<200 GeV. The result is
Gamma(W)=2032 +/- 45(stat)+/-57(syst) MeV, consistent with
the standard model expectation.},
Doi = {10.1103/physrevlett.100.071801},
Key = {fds308021}
}
@article{fds307935,
Author = {al, TAE},
Title = {``Search for the supersymmetric partner of the top quark in
\pbp collisions at $\sqrt{s} = 1.8$ TeV,''},
Journal = {Physical Review},
Volume = {D63},
Number = {9},
Pages = {091101},
Year = {2001},
url = {http://dx.doi.org/10.1103/PhysRevD.63.091101},
Abstract = {We report on a search for the supersymmetric partner of the
top quark (top squark) produced in [Formula Presented]
events using [Formula Presented] of [Formula Presented]
collisions at [Formula Presented] recorded with the Collider
Detector at Fermilab. In the case of a light top squark, the
decay of the top quark into a top squark plus the lightest
supersymmetric particle (LSP) could have a significant
branching ratio. The observed events are consistent with
standard model [Formula Presented] production and decay.
Hence, we set limits on the branching ratio of the top quark
decaying into a top squark plus LSP, excluding branching
ratios above 45% for a LSP mass up to [Formula Presented] ©
2001 The American Physical Society.},
Doi = {10.1103/PhysRevD.63.091101},
Key = {fds307935}
}
@article{fds308022,
Author = {Aaltonen, and T, and others},
Title = {{Cross Section Constrained Top Quark Mass Measurement from
Dilepton Events at the Tevatron}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {6},
Pages = {062005},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.062005},
Abstract = {We report the first top-quark mass measurement that uses a
cross-section constraint to improve the mass determination.
This measurement is made with a dilepton $t\bar{t}$ event
candidate sample collected with the Collider Detector II at
Fermilab. From a data sample corresponding to an integrated
luminosity of 1.2 fb-1, we measure a top-quark mass of
170.7-3.9+4.2(stat)\pm 2.6(syst)\pm 2.4(theory) GeV/c2. The
measurement without the cross-section constraint is
169.7-4.9+5.2(stat)\pm 3.1(syst) GeV/c2.},
Doi = {10.1103/physrevlett.100.062005},
Key = {fds308022}
}
@article{fds308045,
Author = {Aaltonen, and T, and others},
Title = {{Cross section measurements of high-pT dilepton final-state
processes using a global fitting method}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {1},
Pages = {012003},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.012003},
Abstract = {We present a new method for studying high-pT dilepton events
$(e^\pm e^{-/+}, \mu^\pm \mu^{-/+}, e^\pm\mu^{-/+})$ and
simultaneously extracting the production cross sections of
$p\bar{p}$-->$t\bar{t}$, $p\bar{p}$-->W+W-, and
$p\bar{p}$-->Z0-->tau+tau- at a center-of-mass energy of
$\sqrt{s}=1.96$ TeV. We perform a likelihood fit to the
dilepton data in a parameter space defined by the missing
transverse energy and the number of jets in the event. Our
results, which use 360 pb-1 of data recorded with the CDF II
detector at the Fermilab Tevatron Collider, are
sigma($t\bar{t}$)=8.5-2.2+2.7 pb, sigma(W+W-)=16.3-4.4+5.2
pb, and sigma(Z0-->tau+tau-)=291-46+50 pb.},
Doi = {10.1103/PhysRevD.78.012003},
Key = {fds308045}
}
@article{fds308017,
Author = {Aaltonen, and T, and others},
Title = {{Evidence for D0-D0bar mixing using the CDF II
Detector}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {12},
Pages = {121802},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.121802},
Abstract = {We measure the time dependence of the ratio of decay rates
for the rare decay D0-->K+pi- to the Cabibbo-favored decay
D0-->K-pi+. A signal of 12.7×103 D0-->K+pi- decays was
obtained using the Collider Detector at Fermilab II detector
at the Fermilab Tevatron with an integrated luminosity of
1.5 fb-1. We measure the D0-[overline D]0 mixing parameters
(RD,y[prime],x[prime]2), and find that the data are
inconsistent with the no-mixing hypothesis with a
probability equivalent to 3.8 Gaussian standard
deviations.},
Doi = {10.1103/physrevlett.100.121802},
Key = {fds308017}
}
@article{fds308014,
Author = {Aaltonen, and T, and others},
Title = {{First Flavor-Tagged Determination of Bounds on Mixing-
Induced CP Violation in Bs -> J/psi phi Decays}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {16},
Pages = {161802},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.161802},
Abstract = {This Letter describes the first determination of bounds on
the CP-violation parameter 2betas using Bs0 decays in which
the flavor of the bottom meson at production is identified.
The result is based on approximately 2000 Bs0-->J/psiphi
decays reconstructed in a 1.35 fb-1 data sample collected
with the CDF II detector using $p\bar{p}$ collisions
produced at the Fermilab Tevatron. We report confidence
regions in the two-dimensional space of 2betas and the
decay-width difference DeltaGamma. Assuming the standard
model predictions of 2betas and DeltaGamma, the probability
of a deviation as large as the level of the observed data is
15%, corresponding to 1.5 Gaussian standard
deviations.},
Doi = {10.1103/physrevlett.100.161802},
Key = {fds308014}
}
@article{fds308024,
Author = {Aaltonen, and T, and others},
Title = {{First observation of the decay $B^0_s \to D^-_s D^+_s$ and
measurement of its branching ratio}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {2},
Pages = {021803},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.021803},
Abstract = {We report the observation of the exclusive decay
Bs0-->Ds-Ds+ at the 7.5 standard deviation level using 355
pb-1 of data collected by the CDF II detector in $p\bar{p}$
collisions at $\sqrt{s}=1.96$ TeV at the Fermilab Tevatron.
We measure the relative branching ratio [script
B](Bs0-->Ds-Ds+)/[script B](B0-->D-Ds+) =1.44-0.44+0.48.
Using the world average value for [script B](B0-->D-Ds+), we
find [script B](Bs0-->Ds-Ds+) =(9.4-4.2+4.4)×10-3. This
provides a lower bound DeltaGammasCP/Gammas> =2[script
B](Bs0-->Ds-Ds+)>1.2×10-2 at 95% C.L.},
Doi = {10.1103/physrevlett.100.021803},
Key = {fds308024}
}
@article{fds308005,
Author = {Aaltonen, and T, and others},
Title = {{Forward-Backward Asymmetry in Top Quark Production in
$p\bar{p}$ Collisions at $sqrt{s}=1.96$ TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {101},
Number = {20},
Pages = {202001},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.202001},
Abstract = {We present measurements of the forward-backward charge
asymmetry in top pair production using 1.9 fb-1 of
$p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV recorded with
the Collider Detector at Fermilab II. Correcting for
acceptance and measurement dilutions we obtain parton-level
asymmetries of AFB$p\bar{p}$=0.17\pm 0.08 in the $p\bar{p}$
frame and AFB$t\bar{t}$=0.24+/-0.14 in the $t\bar{t}$ frame.
The values are consistent with the standard model
expectation and disfavor exotic production mechanisms with
significant negative values.},
Doi = {10.1103/physrevlett.101.202001},
Key = {fds308005}
}
@article{fds308038,
Author = {Aaltonen, and T, and others},
Title = {{Limits on the Production of Narrow $t\bar{t}$ Resonances in
$p\bar{p}$ Collisions at $\sqrt{s}=1.96$
TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {5},
Pages = {051102},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.051102},
Abstract = {We search for evidence of resonant top quark pair production
in 955 pb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
recorded with the CDF II detector at the Fermilab Tevatron.
For fully reconstructed candidate $t\bar{t}$ events
triggered on leptons with large transverse momentum and
containing at least one identified b-quark jet, we compare
the invariant mass spectrum of $t\bar{t}$ pairs to the
expected superposition of standard model $t\bar{t}$,
non-$t\bar{t}$ backgrounds, and a simple resonance model
based on a sequential Z[prime] boson. We establish upper
limits for sigma($p\bar{p}$-->Z[prime])·Br(Z[prime]-->$t\bar{t}$)
in the Z[prime] mass interval from 450 GeV/c2 to 900 GeV/c2.
A topcolor leptophobic Z[prime] is ruled out below 720
GeV/c2, and the cross section of any narrow Z[prime]-like
state decaying to $t\bar{t}$ is found to be less than 0.64
pb at 95% C.L. for MZ[prime] above 700 GeV/c2.},
Doi = {10.1103/PhysRevD.77.051102},
Key = {fds308038}
}
@article{fds308043,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of $b$-jet Shapes in Inclusive Jet Production
in $p \bar{p}$ Collisions at $\sqrt{s}$ =
1.96-TeV}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {7},
Pages = {072005},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.072005},
Abstract = {We present a measurement of the shapes of b-jets using 300
pb-1 of data obtained with the upgraded Collider Detector at
Fermilab (CDF II) in $p \bar{p}$ collisions at
center-of-mass energy $\sqrt{s}=1.96$ TeV. This measurement
covers a wide transverse momentum range, from 52 to 300
GeV/c. Samples of heavy-flavor enhanced jets together with
inclusive jets are used to extract the average shapes of
b-jets. The b-jets are expected to be broader than inclusive
jets. Moreover, b-jets containing a single b-quark are
expected to be narrower than those containing a $b \bar{b}$
pair from gluon splitting. The measured b-jet shapes are
found to be significantly broader than expected from the
pythia and herwig Monte Carlo simulations. This effect may
arise from an underestimation of the fraction of b-jets
originating from gluon splitting in these simulations. The
jet shape distributions provided in this paper could be
compared to any full Monte Carlo simulation and could be
used to further constrain the various parameters.},
Doi = {10.1103/PhysRevD.78.072005},
Key = {fds308043}
}
@article{fds308026,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of correlated b-bbar production in ${p
\bar{p}}$ collisions at s**(1/2) = 1960 GeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {7},
Pages = {072004},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.072004},
Abstract = {We present a measurement of the correlated b[overline b]
production cross section. The data used in this analysis
were taken with the upgraded CDF detector (CDF II) at the
Fermilab Tevatron collider, and correspond to an integrated
luminosity of 742 pb-1. We utilize muon pairs with invariant
mass 5=3 GeV/c and |eta|=2 GeV/c and |y| mu,[overline b] -->
mu=1549\pm 133 pb. We compare this result with theoretical
predictions and previous measurements. We also report the
measurement of sigmac --> mu,[overline c] --> mu, a
by-product of the study of the background to b[overline b]
production.},
Doi = {10.1103/PhysRevD.77.072004},
Key = {fds308026}
}
@article{fds308018,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of Inclusive Jet Cross Sections in $Z/\gamma^*
(\to ee)+$ jets Production in $p\bar{p}$ Collisions at
$\sqrt{s}=1.96$ TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {10},
Pages = {102001},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.102001},
Abstract = {Inclusive jet cross sections in Z/gamma* events, with
Z/gamma* decaying into an electron-positron pair, are
measured as a function of jet transverse momentum and jet
multiplicity in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
with the upgraded Collider Detector at Fermilab in run II,
based on an integrated luminosity of 1.7 fb-1. The
measurements cover the rapidity region |yjet|Tjet>30 GeV/c.
Next-to-leading order perturbative QCD predictions are in
good agreement with the measured cross sections.},
Doi = {10.1103/physrevlett.100.102001},
Key = {fds308018}
}
@article{fds308016,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of Lifetime and Decay-Width Difference in
$B^0_s \to J/\psi \phi$ Decays}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {12},
Pages = {121803},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.121803},
Abstract = {We measure the mean lifetime ${\tau=2/(\Gamma_L+\Gamma_H)}$
and the decay-width difference ${\Delta\Gamma=\Gamma_L-\Gamma_H}$
of the light and heavy mass eigenstates of the ${B_s^0}$
meson, ${B_{sL}^0}$ and ${B_{sH}^0}$, in ${B_s^0\to
J/\psi\phi}$ decays using 1.7 fb-1 of data collected with
the CDF II detector at the Fermilab Tevatron $p\bar{p}$
collider. Assuming CP conservation, a good approximation for
the ${B_s^0}$ system in the standard model, we obtain
${\Delta\Gamma=0.076_{-0.063}^{+0.059}}$(stat)$\pm
0.006$(syst) ps-1 and $\tau=1.52\pm 0.04$(stat)$\pm
0.02$(syst) ps, the most precise measurements to date. Our
constraints on the weak phase and ${\Delta\Gamma}$ are
consistent with CP conservation.},
Doi = {10.1103/physrevlett.100.121803},
Key = {fds308016}
}
@article{fds308032,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of Ratios of Fragmentation Fractions for Bottom
Hadrons in $p \bar{p}$ Collisions at $\sqrt{s}$ =
1.96-TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {7},
Pages = {072003},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.072003},
Abstract = {This paper describes the first measurement of b-quark
fragmentation fractions into bottom hadrons in Run II of the
Tevatron Collider at Fermilab. The result is based on a 360
pb-1 sample of data collected with the CDF II detector in
$p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV. Semileptonic
decays of [overline B]0, B-, and [overline B]s0 mesons, as
well as Lambdab0 baryons, are reconstructed. For an
effective bottom hadron pT threshold of 7 GeV/c, the
fragmentation fractions are measured to be fu/fd=1.054\pm
0.018(stat)-0.045+0.025(sys)\pm 0.058([script B]),
fs/(fu+fd)=0.160\pm 0.005(stat)-0.010+0.011(sys)-0.034+0.057([script
B]), and fLambdab/(fu+fd)=0.281\pm 0.012(stat)-0.056+0.058(sys)-0.087+0.128([script
B]), where the uncertainty [script B] is due to
uncertainties on measured branching ratios. The value of
fs/(fu+fd) agrees within one standard deviation with
previous CDF measurements and the world average of this
quantity, which is dominated by LEP measurements. However,
the ratio fLambdab/(fu+fd) is approximately twice the value
previously measured at LEP. The approximately 2sigma
discrepancy is examined in terms of kinematic differences
between the two production environments.},
Doi = {10.1103/PhysRevD.77.072003},
Key = {fds308032}
}
@article{fds308041,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of the cross section for ${W}$-boson production
in association with jets in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {6},
Pages = {011108},
Publisher = {American Physical Society (APS)},
Year = {2008},
ISSN = {1550-7998},
url = {http://dx.doi.org/10.1007/JHEP06(2013)084},
Abstract = {We present a measurement of the cross section for W-boson
production in association with jets in $p\bar{p}$ collisions
at $\sqrt{s}=1.96$ TeV. The analysis uses a data sample
corresponding to an integrated luminosity of 320 pb-1
collected with the CDF II detector. W bosons are identified
in their electron decay channel and jets are reconstructed
using a cone algorithm. For each W+>=n-jet sample (n=1-4) we
measure the differential cross section dsigma($p\bar{p}$-->W+>=n-jet)/dETnth-jet×[script
B](W-->enu) with respect to the transverse energy ET of the
nth-highest ET jet above 20 GeV, and the total cross section
sigma($p\bar{p}$-->W+>=n-jet;ETnth-jet>25 GeV)×[script
B](W-->enu), for a restricted W-->enu decay phase space. The
cross sections, corrected for all detector effects, can be
directly compared to particle level W+jet(s) predictions. We
present here comparisons to leading order and
next-to-leading order predictions.},
Doi = {10.1007/JHEP06(2013)084},
Key = {fds308041}
}
@article{fds308044,
Author = {Aaltonen, and T, and others},
Title = {{Measurement of the Inclusive Jet Cross Section at the
Fermilab Tevatron $p \bar{p}$ Collider Using a Cone-Based
Jet Algorithm}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {5},
Pages = {052006},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.052006},
Abstract = {We present a measurement of the inclusive jet cross section
in $p \bar{p}$ collisions at $\sqrt{s}=1.96$ TeV based on
data collected by the CDF II detector with an integrated
luminosity of 1.13 fb-1. The measurement was made using the
cone-based midpoint jet clustering algorithm in the rapidity
region of |y|},
Doi = {10.1103/PhysRevD.78.052006},
Key = {fds308044}
}
@article{fds308029,
Author = {Aaltonen, and T, and others},
Title = {{Model-Independent and Quasi-Model-Independent Search for
New Physics at CDF}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {1},
Pages = {012002},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.012002},
Abstract = {Data collected in run II of the Fermilab Tevatron are
searched for indications of new electroweak scale physics.
Rather than focusing on particular new physics scenarios,
CDF data are analyzed for discrepancies with respect to the
standard model prediction. A model-independent approach
(Vista) considers the gross features of the data and is
sensitive to new large cross section physics. A
quasi-model-independent approach (Sleuth) searches for a
significant excess of events with large summed transverse
momentum and is particularly sensitive to new electroweak
scale physics that appears predominantly in one final state.
This global search for new physics in over 300 exclusive
final states in 927 pb-1 of $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV reveals no such significant indication
of physics beyond the standard model.},
Doi = {10.1103/PhysRevD.78.012002},
Key = {fds308029}
}
@article{fds308034,
Author = {Aaltonen, and T, and others},
Title = {{Observation of Exclusive Dijet Production at the Fermilab
Tevatron ${p \bar{p}}$ Collider}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {5},
Pages = {052004},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.052004},
Abstract = {We present the first observation and cross section
measurement of exclusive dijet production in [overline p]p
interactions, [overline p]p-->[overline p]+dijet+p. Using a
data sample of 310 pb-1 collected by the Run II Collider
Detector at Fermilab at $\sqrt{s}=1.96$ TeV, exclusive cross
sections for events with two jets of transverse energy
ETjet>=10 GeV have been measured as a function of minimum
ETjet. The exclusive signal is extracted from fits to data
distributions based on Monte Carlo simulations of expected
dijet signal and background shapes. The simulated background
distribution shapes are checked in a study of a largely
independent data sample of 200 pb-1 of b-tagged jet events,
where exclusive dijet production is expected to be
suppressed by the Jz=0 total angular momentum selection
rule. Results obtained are compared with theoretical
expectations, and implications for exclusive Higgs boson
production at the pp Large Hadron Collider at sqrt(s)=14 TeV
are discussed.},
Doi = {10.1103/PhysRevD.77.052004},
Key = {fds308034}
}
@article{fds308020,
Author = {Aaltonen, and T, and others},
Title = {{Observation of Orbitally Excited ${B_s}$
Mesons}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {8},
Pages = {082001},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.082001},
Abstract = {We report the observation of two narrow resonances
consistent with states of orbitally excited (L=1) Bs mesons
using 1 fb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
collected with the Collider Detector at Fermilab II detector
at the Fermilab Tevatron. We use two-body decays into K- and
B+ mesons reconstructed as B+-->J/psiK+, J/psi-->\mu^+\mu^-
or B+-->[overline D]0pi+, [overline D]0-->K+pi-. We deduce
the masses of the two states to be m(Bs1)=5829.4\pm 0.7
MeV/c2 and m(Bs2*)=5839.6\pm 0.7 MeV/c2.},
Doi = {10.1103/physrevlett.100.082001},
Key = {fds308020}
}
@article{fds308031,
Author = {Aaltonen, and T, and others},
Title = {{Search for chargino-neutralino production in ${p \bar{p}}$
collisions at 1.96 TeV with high pT leptons}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {5},
Pages = {052002},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.052002},
Abstract = {We present a search for the associated production of
charginos and neutralinos in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV. The data were collected at the Collider
Detector at Fermilab (CDF II) and correspond to integrated
luminosities between 0.7 and 1.0 fb-1. We look for final
states with one high-pT electron or muon, and two additional
leptons. Our results are consistent with the standard model
expectations, and we set limits on the cross section as a
function of the chargino mass in three different
supersymmetric scenarios. For a specific minimal
supersymmetric standard model scenario with no slepton
mixing, we set a 95% C.L. limit at 151 GeV/c2.},
Doi = {10.1103/PhysRevD.77.052002},
Key = {fds308031}
}
@article{fds308009,
Author = {Aaltonen, and T, and others},
Title = {{Search for Doubly Charged Higgs Bosons with Lepton-Flavor-
Violating Decays involving Tau Leptons}},
Journal = {Phys. Rev. Lett.},
Volume = {101},
Number = {12},
Pages = {121801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.121801},
Abstract = {We search for pair production of doubly charged Higgs
particles ($H^{\pm\pm}$) followed by decays into
electron-tau (etau) and muon-tau (mu tau) pairs using data
(350 pb-1) collected from $\bar{p} p$ collisions at
$\sqrt{s}=1.96$ TeV by the CDF II experiment. We search
separately for cases where three or four final-state leptons
are detected, and combine results for exclusive decays to
left-handed etau (\mu tau) pairs. We set an $H^{\pm\pm}$
lower mass limit of 114(112) GeV/c2 at the 95% confidence
level.},
Doi = {10.1103/physrevlett.101.121801},
Key = {fds308009}
}
@article{fds308015,
Author = {Aaltonen, and T, and others},
Title = {{Search for Heavy Top-like Quarks Using Lepton Plus Jets
Events in 1.96-TeV $p \bar{p}$ Collisions}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {16},
Pages = {161803},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.161803},
Abstract = {We present the results of a search for pair production of a
new heavy toplike quark t[prime] decaying to a ${W}$ boson
and another quark using the Collider Detector at Fermilab II
detector in run II of the Tevatron $p\bar{p}$ collider.
Using a data sample corresponding to 760 pb-1 of integrated
luminosity, we fit the observed spectrum of total transverse
energy and reconstructed t[prime] quark mass to a
combination of standard model processes and t[prime] pair
production. We see no evidence for t[prime][overline
t][prime] production, and we infer a lower limit of 256
GeV/c2 on the mass of the t[prime] at 95% C.L. assuming
standard strong couplings for the t[prime].},
Doi = {10.1103/physrevlett.100.161803},
Key = {fds308015}
}
@article{fds308042,
Author = {Aaltonen, and T, and others},
Title = {{Search for Heavy, Long-Lived Neutralinos that Decay to
Photons at CDF II Using Photon Timing}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {3},
Pages = {032015},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.032015},
Abstract = {We present the results of the first hadron collider search
for heavy, long-lived neutralinos that decay via
chi-tilde10-->gammaG-tilde in gauge-mediated supersymmetry
breaking models. Using an integrated luminosity of 570\pm 34
pb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV, we
select gamma+jet+missing transverse energy candidate events
based on the arrival time of a high-energy photon at the
electromagnetic calorimeter as measured with a timing system
that was recently installed on the CDF II detector. We find
2 events, consistent with the background estimate of 1.3\pm
0.7 events. While our search strategy does not rely on
model-specific dynamics, we set cross section limits and
place the world-best 95% C.L. lower limit on the chi-tilde10
mass of 101 GeV/c2 at tauchi-tilde[sub 1][sup 0]=5
ns.},
Doi = {10.1103/PhysRevD.78.032015},
Key = {fds308042}
}
@article{fds308008,
Author = {Aaltonen, and T, and others},
Title = {{Search for large extra dimensions in final states
containing one photon or jet and large missing transverse
energy produced in $p \bar{p}$ collisions at $\sqrt{s}$ =
1.96-TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {101},
Number = {18},
Pages = {181602},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.181602},
Abstract = {We present the results of searches for large extra
dimensions in samples of events with large missing
transverse energy E-slash T and either a photon or a jet
produced in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
collected with the Collider Detector at Fermilab II. For
gamma+E-slash T and jet+E-slash T candidate samples
corresponding to 2.0 and 1.1 fb-1 of integrated luminosity,
respectively, we observe good agreement with standard model
expectations and obtain a combined lower limit on the
fundamental parameter of the large extra dimensions model MD
as a function of the number of extra dimensions in the
model.},
Doi = {10.1103/physrevlett.101.181602},
Key = {fds308008}
}
@article{fds308033,
Author = {Aaltonen, and T, and others},
Title = {{Search for New Heavy Particles Decaying to $Z^0 Z^0 \to
eeee$ in $p$ - $\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-
TeV}},
Journal = {Phys. Rev.},
Volume = {D78},
Number = {1},
Pages = {012008},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.78.012008},
Abstract = {We report the results of a search for the anomalous
production of a massive particle decaying to four electrons
via two Z0 bosons in 1.1 fb-1 of $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV collected by the CDF II detector at
Fermilab. We employ optimized electron identification
criteria to maximize acceptance and efficiency. We estimate
the backgrounds in the invariant mass range 500–1000
GeV/c2 to be 0.028\pm 0.009(stat)\pm 0.011(syst) events. We
observe zero events in this search region. Assuming a
Randall-Sundrum graviton production model, we set 95% C.L.
limits on sigma×BF(G-->Z0Z0)},
Doi = {10.1103/PhysRevD.78.012008},
Key = {fds308033}
}
@article{fds308010,
Author = {Aaltonen, and T, and others},
Title = {{Search for Pair Production of Scalar Top Quarks Decaying to
a $\tau$ Lepton and a $b$ Quark in $p\bar{p}$ Collisions at
sqrt{s}=1.96 TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {101},
Number = {7},
Pages = {071802},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.101.071802},
Abstract = {We search for pair production of supersymmetric top quarks
(t-tilde1), followed by R-parity violating decay
t-tilde1-->taub with a branching ratio beta, using 322 pb-1
of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected by
the upgraded Collider Detector at Fermilab. Two candidate
events pass our final selection criteria, consistent with
the standard model expectation. We set upper limits on the
cross section sigma(t-tilde1[overline t-tilde ]1)×beta2 as
a function of the top-squark mass m(t-tilde1). Assuming
beta=1, we set a 95% confidence level limit m(t-tilde1)>153
GeV/c2. The limits are also applicable to the case of a
third-generation scalar leptoquark (LQ3) decaying
LQ3-->taub.},
Doi = {10.1103/physrevlett.101.071802},
Key = {fds308010}
}
@article{fds308028,
Author = {Aaltonen, and T, and others},
Title = {{Search for resonant $t \bar{t}$ production in $p \bar{p}$
collisions at $\sqrt{s}$ = 1.96-TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {23},
Pages = {231801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.231801},
Abstract = {We report on a search for narrow-width particles decaying to
a top and antitop quark pair. The data set used in the
analysis corresponds to an integrated luminosity of 680 pb-1
collected with the Collider Detector at Fermilab in run II.
We present 95% confidence level upper limits on the cross
section times branching ratio. Assuming a specific
top-color-assisted technicolor production model, the
leptophobic Z[prime] with width GammaZ[prime]=0.012MZ[prime],
we exclude the mass range MZ[prime]},
Doi = {10.1103/physrevlett.100.231801},
Key = {fds308028}
}
@article{fds308023,
Author = {Aaltonen, and T, and others},
Title = {{Search for Standard Model Higgs Bosons Produced in
Association with ${W}$ Bosons}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {4},
Pages = {041801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.041801},
Abstract = {We report the observation of two narrow resonances
consistent with states of orbitally excited (L=1) Bs mesons
using 1 fb-1 of $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV
collected with the Collider Detector at Fermilab II detector
at the Fermilab Tevatron. We use two-body decays into K- and
B+ mesons reconstructed as B+-->J/psiK+, J/psi-->\mu +\mu -
or B+-->[overline D]0pi+, [overline D]0-->K+pi-. We deduce
the masses of the two states to be m(Bs1)=5829.4\pm 0.7
MeV/c2 and m(Bs2*)=5839.6\pm 0.7 MeV/c2.},
Doi = {10.1103/physrevlett.100.041801},
Key = {fds308023}
}
@article{fds308012,
Author = {Aaltonen, and T, and others},
Title = {{Search for the Higgs boson in events with missing
transverse energy and $b$ quark jets produced in proton-
antiproton collisions at $\sqrt{s}$ =1.96
TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {21},
Pages = {211801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.211801},
Abstract = {We search for the standard model Higgs boson produced in
association with an electroweak vector boson in events with
no identified charged leptons, large imbalance in transverse
momentum, and two jets where at least one contains a
secondary vertex consistent with the decay of b hadrons. We
use ~1 fb-1 integrated luminosity of $p\bar{p}$ collisions
at $\sqrt{s}=1.96$ TeV recorded by the Collider Detector at
Fermilab II experiment at the Tevatron. We find 268 (16)
single (double) b-tagged candidate events, where $248\pm 43$
($14.4\pm 2.7$) are expected from standard model background
processes. We observe no significant excess over the
expected background and thus set 95% confidence level upper
limits on the Higgs boson production cross section for
several Higgs boson masses ranging from 110 to 140 GeV/c2.
For a mass of 115 GeV/c2, the observed (expected) limit is
20.4 (14.2) times the standard model prediction.},
Doi = {10.1103/physrevlett.100.211801},
Key = {fds308012}
}
@article{fds308025,
Author = {Aaltonen, and T, and others},
Title = {{Search for third generation vector leptoquarks in
$p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {9},
Pages = {091105},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.091105},
Abstract = {We search for a third generation vector leptoquark (VLQ3)
that decays to a $b$ quark and tau lepton using the CDF II
detector and 320 pb-1 of integrated luminosity from the
Fermilab Tevatron. Observing a number of events in agreement
with standard model expectations, we obtain, assuming
Yang-Mills (minimal) couplings, the most stringent upper
limit on the VLQ3 pair production cross section of 344 fb
(493 fb) and lower limit on the VLQ3 mass of 317 GeV/c2 (251
GeV/c2) at 95% C.L.},
Doi = {10.1103/PhysRevD.77.091105},
Key = {fds308025}
}
@article{fds308013,
Author = {Aaltonen, and T, and others},
Title = {{Strong Evidence for $Z Z$ Production in panti-p Collisions
at $\sqrt{s}$ = 1.96-TeV}},
Journal = {Phys. Rev. Lett.},
Volume = {100},
Number = {20},
Pages = {201801},
Year = {2008},
url = {http://dx.doi.org/10.1103/physrevlett.100.201801},
Abstract = {We report the first evidence of Z boson pair production at a
hadron collider with a significance exceeding 4 standard
deviations. This result is based on a data sample
corresponding to 1.9 fb-1 of integrated luminosity from
$p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV collected with
the Collider Detector at Fermilab II detector. In the
[script-l][script-l][script-l][prime][script-l][prime]
channel, we observe three ZZ candidates with an expected
background of 0.096-0.063+0.092 events. In the
[script-l][script-l]nunu channel, we use a leading-order
calculation of the relative ZZ and WW event probabilities to
discriminate between signal and background. In the
combination of [script-l][script-l][script-l][prime][script-l][prime]
and [script-l][script-l]nunu channels, we observe an excess
of events with a probability of 5.1×10-6 to be due to the
expected background. This corresponds to a significance of
4.4 standard deviations. The measured cross section is
sigma($p\bar{p}$-->ZZ)=1.4-0.6+0.7(stat+syst) pb, consistent
with the standard model expectation.},
Doi = {10.1103/physrevlett.100.201801},
Key = {fds308013}
}
@article{fds308037,
Author = {Aaltonen, and T, and others},
Title = {{Two-particle momentum correlations in jets produced in $p
\bar{p}$ Collisions at $\sqrt{s}$ = 1.96-TeV}},
Journal = {Phys. Rev.},
Volume = {D77},
Number = {9},
Pages = {092001},
Publisher = {American Physical Society (APS)},
Year = {2008},
url = {http://dx.doi.org/10.1103/PhysRevD.77.092001},
Abstract = {We present the first measurement of two-particle momentum
correlations in jets produced in $p\bar{p}$ collisions at
$\sqrt{s}=1.96$ TeV. Results are obtained for charged
particles within a restricted cone with an opening angle of
0.5 radians around the jet axis and for events with dijet
masses between 66 and 563 GeV/c2. A comparison of the
experimental data to theoretical predictions obtained for
partons within the framework of resummed perturbative QCD in
the next-to-leading log approximation shows that the parton
momentum correlations survive the hadronization stage of jet
fragmentation, giving further support to the hypothesis of
local parton-hadron duality. The extracted value of the
next-to-leading-log-approximation parton shower cutoff scale
Qeff set equal to LambdaQCD is found to be
(1.4-0.7+0.9)×100 MeV.},
Doi = {10.1103/PhysRevD.77.092001},
Key = {fds308037}
}
@article{fds308210,
Author = {Adams, MR and Aderholz, M and Aïd, S and Anthony, PL and Ashery, D and Averill, DA and Baker, MD and Baller, BR and Banerjee, A and Bhatti, AA and Bratzler, U and Braun, HM and Carroll, TJ and Clark, HL and Conrad, JM and Davisson, R and Derado, I and Dietrich, FS and Dougherty, W and Dreyer,
T and Eckardt, V and Ecker, U and Erdmann, M and Fang, GY and Figiel, J and Finlay, RW and Gebauer, HJ and Geesaman, DF and Griffioen, KA and Guo,
RS and Haas, J and Halliwell, C and Hantke, D and Hicks, KH and Jackson,
HE and Jancso, G and Jansen, DM and Jin, Z and Kadija, K and Kaufmann, S and Kennedy, RD and Kinney, ER and Kobrak, HGE and Kotwal, AV and Kunori, S and Lenski, M and Lord, JJ and Lubatti, HJ and McLeod, D and Madden, P and Manz, A and Melanson, H and Michael, DG and Montgomery, HE and Morfin,
JG and Nickerson, RB and Novak, J and Olkiewicz, K and Osborne, L and Otten, R and Papavassiliou, V and Pawlik, B and Pipkin, FM and Potterveld, DH and Röser, A and Ryan, JJ and Salgado, CW and Schellman,
H and Schmitt, M and Schmitz, N and Siegert, G and Skuja, A and Snow, GA and Söldner-Rembold, S and Spentzouris, P and Stopa, P and Swanson, RA and Topor Pop and V and Venkataramania, H and Wilhelm, M and Wilson, R and Wittek, W and Wolbers, SA and Zghiche, A and Zhao,
T},
Title = {Λ and Λ̄ polarization from deep inelastic muon
scattering},
Journal = {European Physical Journal C},
Volume = {17},
Number = {2},
Pages = {263-267},
Year = {2000},
Month = {January},
url = {http://dx.doi.org/10.1007/s100520000493},
Abstract = {We report results of the first measurements of Λ and Λ̄
polarization produced in deep inelastic polarized muon
scattering on the nucleon. The results are consistent with
an expected trend towards positive polarization with
increasing cursive Greek chiF. The polarizations of Λ and
Λ̄ appear to have opposite signs. A large negative
polarization for Λ at low positive cursive Greek chiF is
observed and is not explained by existing models. A possible
interpretation is presented.},
Doi = {10.1007/s100520000493},
Key = {fds308210}
}
%% Papers Accepted
@article{fds375049,
Author = {A.V. Kotwal and the ATLAS Collaboration},
Title = {Search for top-philic heavy resonances in pp collisions at
√s = 13 TeV with the ATLAS detector},
Publisher = {European Physics Journal C},
Year = {2023},
Month = {Winter},
url = {https://doi.org/10.48550/arXiv.2304.01678},
Key = {fds375049}
}
%% Papers Submitted
@article{fds354061,
Author = {G. Aad et al (ATLAS Collaboration)},
Title = {Jet energy scale and resolution measured in proton-proton
collisions at √s=13 TeV with the ATLAS
detector},
Journal = {European Physics Journal C},
Year = {2020},
Month = {July},
Key = {fds354061}
}
@article{fds354062,
Author = {G. Aad et al (ATLAS Collaboration)},
Title = {Search for displaced leptons in √s=13 TeV pp collisions
with the ATLAS detector},
Journal = {Physical Review Letters},
Year = {2020},
Month = {November},
Key = {fds354062}
}
%% Preprints
@article{fds347562,
Author = {A.V. Kotwal},
Title = {A fast method for finding charged-particle trajectories
using unsupervised machine learning embedded in
field-programmable gate arrays},
Year = {2019},
Month = {October},
url = {http://arxiv.org/abs/1910.14149v1},
Key = {fds347562}
}
@article{fds221253,
Author = {A.V. Kotwal and the ATLAS Collaboration},
Title = {Beyond Standard Model Higgs boson searches at a
High-Luminosity LHC with ATLAS},
Journal = {ATL-PHYS-PUB-2013-016},
Year = {2013},
Month = {October},
Key = {fds221253}
}
@article{fds221248,
Author = {A.V. Kotwal and the ATLAS Collaboration},
Title = {Studies of Sensitivity to New Dilepton and Ditop Resonances
with an Upgraded ATLAS Detector at a High-Luminosity
LHC},
Journal = {ATLAS-PHYS-PUB-2013-003},
Year = {2013},
Month = {February},
Key = {fds221248}
}
@article{fds221250,
Author = {A.V. Kotwal and the ATLAS Collaboration},
Title = {Studies of Vector Boson Scattering And Triboson Production
with an Upgraded ATLAS Detector at a High-Luminosity
LHC},
Journal = {ATL-PHYS-PUB-2013-006},
Year = {2013},
Month = {June},
Key = {fds221250}
}
@article{fds221249,
Author = {A.V. Kotwal and C. Degrange et al.},
Title = {Studies of Vector Boson Scattering And Triboson Production
with DELPHES Parametrized Fast Simulation for Snowmass
2013},
Journal = {arXiv:1309.7452},
Year = {2013},
Month = {October},
Key = {fds221249}
}